JP2014049319A - Light-emitting device and illumination method - Google Patents

Abstract

PROBLEM TO BE SOLVED: To provide an illumination method and a light-emitting device in which, under an indoor illuminance environment where illuminance is about 5000 lx or less or 1500 lx or less in general while including such a case that a detailed task is performed, regarding a human sensible look of colors, such a natural, vivid, highly visible and comfortable look of colors as under an outdoor high-illuminance environment can be realized regardless of various color rendition metric scores.SOLUTION: A light-emitting device is characterized in that light emitted in a main radiation direction from the light-emitting device meets a specific requirement. When an object is irradiated with light emitted from the light-emitting device, illumination is performed in such a manner that light measured at a position of the object meets the specific requirement.

Description

  The present invention relates to a light emitting device including both a light emitting element and a control element, a design method related to the light emitting device, and a lighting method using the light emitting device.

  In recent years, GaN-based semiconductor light-emitting elements have made remarkable progress in increasing output and efficiency. In addition, high efficiency of semiconductor phosphors or various phosphors using an electron beam as an excitation source has been actively studied. As a result, light-emitting devices such as current light sources, light source modules including light sources, instruments including light source modules, systems including instruments, and the like are rapidly saving power compared to conventional ones.

  For example, a GaN-based blue light-emitting element is included as an excitation light source of a yellow phosphor, and a so-called pseudo-white light source is created from the spectrum of the GaN-based blue light-emitting element and the spectrum of the yellow phosphor, or an illumination light source, or It is widely practiced to use a lighting fixture that includes this, and a lighting system in which a plurality of such fixtures are arranged in a space. (See Patent Document 1)

A packaged LED (for example, the package material includes the GaN-based blue light-emitting element, yellow phosphor, sealant, etc.), which is a kind of illumination light source that can be inherent in these forms, has a correlated color of about 6000K. In the temperature (Correlated Color Temperature / CCT) region, there is a product whose light source efficiency as a package LED exceeds 150 lm / W. (See Non-Patent Document 2)
Furthermore, the efficiency and power saving of liquid crystal backlight light sources are also progressing.

However, it has been pointed out from various directions that these light-emitting devices aiming at high efficiency are insufficient in consideration of color appearance. In particular, when used for illumination, the efficiency of light-emitting devices such as light sources / appliances / systems is improved, and “color appearance (Color) when an object is illuminated”
"Appearance)" is very important.

As an attempt to take these into consideration, in order to improve the score of the Color Rendering Index / CRI (CIE (13.3)) established by the International Lighting Commission (Commission Internationale de I'Eclairage / CIE). Attempts have been made to superimpose a spectrum of a red phosphor or a red semiconductor light emitting element on a spectrum of a blue light emitting element and a spectrum of a yellow phosphor. For example, in a typical spectrum without a red source (CCT = about 6800K), the average color rendering index (R _a ) and the special color rendering index (R ₉ ) for a vivid red color chart are R _a, respectively. = 81, R ₉ = 24, but when a red source is included, the score of the color rendering index can be raised to R _a = 98 and R ₉ = 95. (See Patent Document 2)

  As another attempt, particularly in special lighting applications, the spectrum emitted from the light emitting device is adjusted to make the appearance of the color of the object a desired color. For example, Non-Patent Document 1 describes an illumination light source having a red color tone.

Japanese Patent No. 3503139 WO2011 / 024818 pamphlet

“General fluorescent lamp Meat-kun”, [online], Prince Electric Co., Ltd. [searched on May 16, 2011], Internet <URL: http://www.prince-d.co.jp/pdct/docs/ pdf / catalog_pdf / fl_nrb_ca2011.pdf> “LEDs MAGAZINE, [searched on August 22, 2011], Internet <URL: http://www.ledsmagazine.com/news/8/8/2>

The color rendering index is the color when illuminated with test light against the appearance of the color illuminated with “reference light” selected corresponding to the CCT of the light (test light) of the light emitting device to be evaluated. It is an index showing how close the appearance of the is. That is, the color rendering index is an index indicating the fidelity of the light emitting device to be evaluated. However, it is not necessarily human that the average color rendering index (R _a ) or special color rendering index (R _i (i is 1 to 14, i is 1 to 15 according to JIS regulations in Japan)) is high. It is becoming clear that it does not induce good color perception. That is, there is a problem that these methods for improving the score of the color rendering evaluation number do not necessarily realize a good color appearance.

  Further, the effect of changing the color appearance according to the illuminance of the illuminated object is not included in various current color rendering metrics. When the bright flower color seen outdoors, which usually has an illuminance of about 10000 lx or more, is brought into a room of about 500 lx, it appears to be a different color with a dull color and a reduced saturation even though it is essentially the same color. That is usually experienced. In general, the degree of saturation related to the appearance of the color of an object depends on the illuminance, and the degree of saturation decreases as the illuminance decreases even if the illuminated spectral distribution is the same. That is, the color appearance is dull. This is known as the Hunt effect.

  Although the hunt effect greatly affects the color rendering properties, it is not actively considered in the evaluation of light emitting devices such as current light sources, fixtures, and systems. The simplest compensation method for the hunt effect is to extremely increase the room illuminance, but this unnecessarily increases the energy consumption. In particular, how to achieve natural, lively, highly visible, comfortable color appearance and object appearance as seen outdoors, with illuminance comparable to an indoor lighting environment. It is not clear whether it can be done.

  On the other hand, for special lighting such as restaurants and food lighting, for example, in light whose spectrum is adjusted in the direction of increasing the saturation of red, yellow appears reddish compared to the reference light, blue is green There are problems such as a large hue (angle) shift, such as appearing. That is, the appearance of colors other than those limited as illumination objects will not be natural. In addition, when a white object is illuminated with such light, the white object itself is colored and does not appear white.

In order to solve the above-mentioned problems, the present inventor, in Japanese Patent Application No. 2011-223472, etc., has a room illuminance that is about 5000 lx or less, or generally about 1500 lx or less, including the case where fine work is performed. Under the environment, human-perceived color appearance is natural, lively, and visible as seen in an outdoor high-light environment, regardless of the scores of various color rendering metrics. The present invention has reached the invention of illumination methods that can realize high, comfortable, color appearance, and object appearance, and light emitting devices such as illumination light sources, lighting fixtures, and illumination systems. The present inventor has also reached a lighting method that simultaneously realizes a comfortable lighting environment with high efficiency. Furthermore, the present inventor has reached a design guideline for such a preferable light emitting device.

However, even if the excellent light-emitting device and illumination method as described above or the design guidelines for realizing this are followed, further contrivance may be required depending on the relative spectral distribution of the light-emitting device. For example, even if a light-emitting device having the above-described excellent characteristics is realized, if an art object is an object to be illuminated, or an article of clothing using a dye that is noticeably faded by light is an object to be illuminated. In such a case, depending on the relative spectral distribution of the light emitting device, there is a risk of accelerating these deteriorations. Even when a light-emitting device having the above-described excellent characteristics is realized, when fresh food or the like is an object to be illuminated, there is a risk that these freshnesses may be deteriorated depending on the relative spectral distribution of the light-emitting device. is there.
The main object of the present invention is to provide a light-emitting device that can cope with such individual specific requests in addition to the above-described invention that the present inventors have already achieved.

［１９］［１］から［１７］のいずれかに記載の発光装置であって、
前記φ_ＳＳＬ（λ）から導出される光の相関色温度Ｔ_ＳＳＬ（Ｋ）に応じて選択される基準の光の分光分布をφ_ｒｅｆ（λ）、前記発光装置から当該放射方向に出射される光の三刺激値を（Ｘ_ＳＳＬ、Ｙ_ＳＳＬ、Ｚ_ＳＳＬ）、前記発光装置から当該放射方向に出射される光のＴ_ＳＳＬ（Ｋ）に応じて選択される基準の光の三刺激値を（Ｘ_ｒｅｆ、Ｙ_ｒｅｆ、Ｚ_ｒｅｆ）とし、
前記発光装置から当該放射方向に出射される光の規格化分光分布Ｓ_ＳＳＬ（λ）と、前記発光装置から当該放射方向に出射される光のＴ_ＳＳＬ（Ｋ）に応じて選択される基準の光の規格化分光分布Ｓ_ｒｅｆ（λ）と、これら規格化分光分布の差ΔＳ（λ）をそれぞれ、
Ｓ_ＳＳＬ（λ）＝φ_ＳＳＬ（λ）／Ｙ_ＳＳＬ
Ｓ_ｒｅｆ（λ）＝φ_ｒｅｆ（λ）／Ｙ_ｒｅｆ
ΔＳ（λ）＝Ｓ_ｒｅｆ（λ）−Ｓ_ＳＳＬ（λ）
と定義し、
波長３８０ｎｍ以上７８０ｎｍ以内の範囲で、Ｓ_ＳＳＬ（λ）の最長波長極大値を与える波長をλ_Ｒ（ｎｍ）とした際に、λ_Ｒよりも長波長側にＳ_ＳＳＬ（λ_Ｒ）／２となる波長Λ４が存在せず、
下記数式（２）で表される指標Ａ_ｃｇが、−３６０ ≦ Ａ_ｃｇ ≦ −１０を満たす
こと
を特徴とする発光装置。

［２０］［１８］または［１９］に記載の発光装置であって、
前記発光装置から当該放射方向に出射される光が以下の（１）及び（２）を満たすことを特徴とする発光装置。
（１）前記発光装置から当該放射方向に出射される光による照明を数学的に仮定した場合の＃０１から＃１５の下記１５種類の修正マンセル色票のＣＩＥ １９７６ Ｌ^*ａ^*ｂ^*
色空間におけるａ^*値、ｂ^*値をそれぞれａ^* _ｎＳＳＬ、ｂ^* _ｎＳＳＬ（ただしｎは１から１５の自然数）とし、
当該放射方向に出射される光の相関色温度Ｔ_ＳＳＬ（Ｋ）に応じて選択される基準の光での照明を数学的に仮定した場合の当該１５種類の修正マンセル色票のＣＩＥ １９７６
Ｌ^*ａ^*ｂ^*色空間におけるａ^*値、ｂ^*値をそれぞれａ^* _ｎｒｅｆ、ｂ^* _ｎｒｅｆ（ただし
ｎは１から１５の自然数）とした場合に、飽和度差ΔＣ_ｎが
−３．８ ≦ ΔＣ_ｎ ≦ １８．６ （ｎは１から１５の自然数）
を満たし、下記式（３）で表される飽和度差の平均が下記式（４）を満たし、

かつ飽和度差の最大値をΔＣ_ｍａｘ、飽和度差の最小値をΔＣ_ｍｉｎとした場合に、飽和度差の最大値と、飽和度差の最小値との間の差ΔＣ_ｍａｘ−ΔＣ_ｍｉｎが
２．８ ≦ （ΔＣ_ｍａｘ−ΔＣ_ｍｉｎ） ≦ １９．６
を満たす。
ただし、ΔＣ_n＝√｛（ａ^* _ｎＳＳＬ）^２＋（ｂ^* _ｎＳＳＬ）^２｝−√｛（ａ^* _ｎｒｅｆ）^２＋（ｂ^* _ｎｒｅｆ）^２｝とする。
１５種類の修正マンセル色票
＃０１ ７．５ Ｐ ４ ／１０
＃０２ １０ ＰＢ ４ ／１０
＃０３ ５ ＰＢ ４ ／１２
＃０４ ７．５ Ｂ ５ ／１０
＃０５ １０ ＢＧ ６ ／ ８
＃０６ ２．５ ＢＧ ６ ／１０
＃０７ ２．５ Ｇ ６ ／１２
＃０８ ７．５ ＧＹ ７ ／１０
＃０９ ２．５ ＧＹ ８ ／１０
＃１０ ５ Ｙ ８．５／１２
＃１１ １０ ＹＲ ７ ／１２
＃１２ ５ ＹＲ ７ ／１２
＃１３ １０ Ｒ ６ ／１２
＃１４ ５ Ｒ ４ ／１４
＃１５ ７．５ ＲＰ ４ ／１２
（２）前記発光装置から当該放射方向に出射される光による照明を数学的に仮定した場合の上記１５種類の修正マンセル色票のＣＩＥ １９７６ Ｌ^*ａ^*ｂ^*色空間における色相
角をθ_ｎＳＳＬ（度）（ただしｎは１から１５の自然数）とし、
当該放射方向に出射される光の相関色温度Ｔ_ＳＳＬ（Ｋ）に応じて選択される基準の光での照明を数学的に仮定した場合の当該１５種類の修正マンセル色票のＣＩＥ １９７６
Ｌ^*ａ^*ｂ^*色空間における色相角をθ_ｎｒｅｆ（度）（ただしｎは１から１５の自然数
）とした場合に、色相角差の絶対値｜Δｈ_ｎ｜が
０ ≦ ｜Δｈ_ｎ｜ ≦ ９．０（度）（ｎは１から１５の自然数）
を満たす。
ただし、Δｈ_ｎ＝θ_ｎＳＳＬ−θ_ｎｒｅｆとする。
［２１］［１８］〜［２０］のいずれかに記載の発光装置であって、
前記発光装置から当該放射方向に出射される光は、分光分布φ_ＳＳＬ（λ）から導出される波長３８０ｎｍ以上７８０ｎｍ以下の範囲の放射効率Ｋ（ｌｍ／Ｗ）が
１８０（ｌｍ／Ｗ） ≦ Ｋ（ｌｍ／Ｗ） ≦ ３２０（ｌｍ／Ｗ）
を満たすことを特徴とする発光装置。
［２２］［２０］に記載の発光装置であって、前記色相角差の絶対値｜Δｈ_ｎ｜が
０．０００３ ≦ ｜Δｈ_ｎ｜ ≦ ８．３（度）（ｎは１から１５の自然数）
を満たすことを特徴とする発光装置。
［２３］［２０］に記載の発光装置であって、前記一般式（３）で表される飽和度差の平均が下記式（４）´を満たすことを特徴とする発光装置。

（４）´
［２４］［２０］に記載の発光装置であって、前記飽和度差ΔＣ_ｎが
−３．４ ≦ ΔＣ_ｎ ≦ １６．８ （ｎは１から１５の自然数）
を満たすことを特徴とする発光装置。
［２５］［２０］に記載の発光装置であって、前記飽和度差の最大値と、前記飽和度差の最小値との間の差ΔＣ_ｍａｘ−ΔＣ_ｍｉｎが
３．２ ≦ （ΔＣ_ｍａｘ−ΔＣ_ｍｉｎ） ≦ １７．８
を満たすことを特徴とする発光装置。
［２６］［１８］〜［２５］のいずれかに記載の発光装置であって、
前記発光装置から当該放射方向に出射される光は、黒体放射軌跡からの距離Ｄ_{ｕｖＳＳＬ}が
−０．０２５０ ≦ Ｄ_{ｕｖＳＳＬ} ≦ −０．０１００
を満たすことを特徴とする発光装置。
［２７］［１８］〜［２６］のいずれかに記載の発光装置であって、前記数式（１）または（２）で表される指標Ａ_ｃｇが
−３２２ ≦ Ａ_ｃｇ ≦ −１２
を満たすことを特徴とする発光装置。
［２８］［１８］〜［２７］のいずれかに記載の発光装置であって、
前記発光装置から当該放射方向に出射される光は、分光分布φ_ＳＳＬ（λ）から導出される波長３８０ｎｍ以上７８０ｎｍ以下の範囲の放射効率Ｋ（ｌｍ／Ｗ）が、
２０６（ｌｍ／Ｗ） ≦ Ｋ（ｌｍ／Ｗ） ≦ ２８８（ｌｍ／Ｗ）
を満たすことを特徴とする発光装置。
［２９］［１８］〜［２８］のいずれかに記載の発光装置であって、前記相関色温度Ｔ_ＳＳＬ（Ｋ）が
２５５０（Ｋ） ≦ Ｔ_ＳＳＬ（Ｋ） ≦ ５６５０（Ｋ）
を満たすことを特徴とする発光装置。
［３０］［１８］〜［２９］のいずれかに記載の発光装置であって、前記発光装置から当該放射方向に出射される光が対象物を照明する照度が１５０ｌｘ以上５０００ｌｘ以下であることを特徴とする発光装置。
［３１］［１８］〜［３０］のいずれかに記載の発光装置であって、前記発光装置は１種類以上６種類以下の発光要素から出射される光を当該放射方向に発することを特徴とする発光装置。
［３２］［１８］〜［３１］のいずれかに記載の発光装置であって、前記発光装置は発光要素として半導体発光素子を含み、前記半導体発光素子の発光スペクトルのピーク波長が３８０ｎｍ以上４９５ｎｍ未満であって、かつ、半値全幅が２ｎｍ以上４５ｎｍ以下であることを特徴とする発光装置。
［３３］［３２］に記載の発光装置であって、前記半導体発光素子の発光スペクトルのピーク波長が３９５ｎｍ以上４２０ｎｍ未満であることを特徴とする発光装置。
［３４］［３２］に記載の発光装置であって、前記半導体発光素子の発光スペクトルのピーク波長が４２０ｎｍ以上４５５ｎｍ未満であることを特徴とする発光装置。
［３５］［３２］に記載の発光装置であって、当該半導体発光素子の発光スペクトルのピーク波長が４５５ｎｍ以上４８５ｎｍ未満であることを特徴とする発光装置。
［３６］［１８］〜［３１］のいずれかに記載の発光装置であって、前記発光装置は発光要素として半導体発光素子を含み、前記半導体発光素子の発光スペクトルのピーク波長が４９５ｎｍ以上５９０ｎｍ未満であって、かつ、半値全幅が２ｎｍ以上７５ｎｍ以下であることを特徴とする発光装置。
［３７］［１８］〜［３１］のいずれかに記載の発光装置であって、前記発光装置は発光要素として半導体発光素子を含み、前記半導体発光素子の発光スペクトルのピーク波長が５９０ｎｍ以上７８０ｎｍ未満であって、かつ、半値全幅が２ｎｍ以上３０ｎｍ以下であることを特徴とする発光装置。
［３８］［１８］〜［３１］のいずれかに記載の発光装置であって、前記発光装置は発光要素として半導体発光素子を含み、前記半導体発光素子はサファイア基板、ＧａＮ基板、ＧａＡｓ基板、ＧａＰ基板からなる群から選択されるいずれかの基板上で作成されたことを特徴とする発光装置。
［３９］［１８］〜［３１］のいずれかに記載の発光装置であって、前記発光装置は発光要素として半導体発光素子を含み、前記半導体発光素子はＧａＮ基板、またはＧａＰ基板上で作成され、かつ前記基板の厚みが１００μｍ以上２ｍｍ以下であることを特徴とする発光装置。
［４０］［１８］〜［３２］のいずれかに記載の発光装置であって、前記発光装置は発光要素として半導体発光素子を含み、前記半導体発光素子はサファイア基板、またはＧａＡｓ基板上で作成され、かつ半導体発光素子は基板から剥離されてなることを特徴とする発光装置。
［４１］［１８］〜［３５］のいずれかに記載の発光装置であって、発光要素として蛍光体を備えることを特徴とする発光装置。
［４２］［４１］に記載の発光装置であって、前記蛍光体は、発光スペクトルの異なる蛍光体を１種類以上５種類以下含むことを特徴とする発光装置。
［４３］［４１］または［４２］に記載の発光装置であって、前記蛍光体は、室温で光励起した場合の単体発光スペクトルのピーク波長が３８０ｎｍ以上４９５ｎｍ未満であって、かつ、半値全幅が２ｎｍ以上９０ｎｍ以下である蛍光体を含むことを特徴とする発光装置。
［４４］［４３］に記載の発光装置であって、前記蛍光体が下記一般式（５）で表される蛍光体、下記一般式（５）´で表される蛍光体、（Ｓｒ，Ｂａ）_３ＭｇＳｉ_２Ｏ_８：Ｅｕ^２＋、および（Ｂａ，Ｓｒ，Ｃａ，Ｍｇ）Ｓｉ_２Ｏ_２Ｎ_２：Ｅｕからなる群から選択される１種以上を含むことを特徴とする発光装置。
（Ｂａ、Ｓｒ、Ｃａ）ＭｇＡｌ_１０Ｏ_１７：Ｍｎ，Ｅｕ （５）
Ｓｒ_ａＢａ_ｂＥｕ_ｘ（ＰＯ_４）_ｃＸ_ｄ （５）´
（一般式（５）´において、ＸはＣｌである。また、ｃ、ｄ及びｘは、２．７≦ｃ≦３．３、０．９≦ｄ≦１．１、０．３≦ｘ≦１．２を満足する数である。さらに、ａ及びｂは、ａ+ｂ＝５−ｘかつ０≦ｂ／（ａ＋ｂ）≦０．６の条件を満足する。）
［４５］［４１］または［４２］に記載の発光装置であって、前記蛍光体は、室温で光励起した場合の単体発光スペクトルのピーク波長が４９５ｎｍ以上５９０ｎｍ未満であって、かつ、半値全幅が２ｎｍ以上１３０ｎｍ以下である蛍光体を含むことを特徴とする発光装置。
［４６］［４５］に記載の発光装置であって、前記蛍光体がＳｉ_６−ｚＡｌ_ｚＯ_ｚＮ_８−ｚ：Ｅｕ（ただし０＜ｚ＜４．２）、下記一般式（６）で表される蛍光体、下記一般式（６）´で表される蛍光体、およびＳｒＧａＳ_４：Ｅｕ^２＋からなる群から選択される１種以上を含むことを特徴とする発光装置。
（Ｂａ_ａＣａ_ｂＳｒ_ｃＭｇ_ｄＥｕ_ｘ）ＳｉＯ_４ （６）
（一般式（６）においてａ、ｂ、ｃ、ｄおよびｘが、ａ＋ｂ＋ｃ＋ｄ＋ｘ＝２、１．０ ≦ ａ ≦ ２．０、０ ≦ ｂ ＜ ０．２、０．２ ≦ ｃ ≦ ０．８、０ ≦ ｄ ＜ ０．２
および０ ＜ ｘ ≦ ０．５を満たす。）
Ｂａ_{１−ｘ−ｙ} Ｓｒ_ｘ Ｅｕ_ｙ Ｍｇ_１−ｚ Ｍｎ_ｚ Ａｌ_１０Ｏ_１７ （６）´
（一般式（６）´においてｘ、ｙおよびｚはそれぞれ０．１≦ｘ≦０．４、０．２５≦ｙ≦０．６及び０．０５≦ｚ≦０．５を満たす。）
［４７］［４１］または［４２］に記載の発光装置であって、前記蛍光体は、室温で光励起した場合の単体発光スペクトルのピーク波長が５９０ｎｍ以上７８０ｎｍ未満であって、かつ、半値全幅が２ｎｍ以上１３０ｎｍ以下である蛍光体を含むことを特徴とする発光装置。
［４８］［４７］に記載の発光装置であって、前記蛍光体が下記一般式（７）で表される蛍光体、下記一般式（７）´で表される蛍光体、（Ｓｒ，Ｃａ，Ｂａ）_２Ａｌ_ｘＳｉ_５−ｘＯ_ｘＮ_８−ｘ：Ｅｕ（ただし０≦ｘ≦２）、Ｅｕ_ｙ（Ｓｒ，Ｃａ，Ｂａ）_１−ｙ：Ａｌ_１＋ｘＳｉ_４−ｘＯ_ｘＮ_７−ｘ（ただし０≦ｘ＜４、０≦ｙ＜０．２）、Ｋ_２ＳｉＦ_６：Ｍｎ^４＋、Ａ_２＋ｘＭ_ｙＭｎ_ｚＦ_ｎ（ＡはＮａおよび／またはＫ；ＭはＳｉおよびＡｌ；−１≦ｘ≦１かつ０．９≦ｙ＋ｚ≦１．１かつ０．００１≦ｚ≦０．４かつ５≦ｎ≦７）、（Ｃａ，Ｓｒ，Ｂａ，Ｍｇ）ＡｌＳｉＮ_３：Ｅｕおよび／または（Ｃａ，Ｓｒ，Ｂａ）ＡｌＳｉＮ_３：Ｅｕ、並びに（ＣａＡｌＳｉＮ_３）_１−ｘ（Ｓｉ_２Ｎ_２Ｏ）_ｘ：Ｅｕ（ただし、ｘは０＜ｘ＜０．５）からなる群から選択される１種以上を含むことを特徴とする発光装置。
（Ｌａ_{１−ｘ−ｙ}，Ｅｕ_ｘ，Ｌｎ_ｙ）_２Ｏ_２Ｓ （７）
（一般式（７）において、ｘ及びｙはそれぞれ０．０２≦ｘ≦０．５０及び０≦ｙ≦０．５０を満たす数を表し、ＬｎはＹ、Ｇｄ、Ｌｕ、Ｓｃ、Ｓｍ及びＥｒの少なくとも１種の３価希土類元素を表す。）
（ｋ−ｘ）ＭｇＯ・ｘＡＦ_２・ＧｅＯ_２：ｙＭｎ^４＋ （７）´
（一般式（７）´において、ｋ、ｘ、ｙは、各々、２．８≦ｋ≦５、０．１≦ｘ≦０．７、０．００５≦ｙ≦０．０１５を満たす数を表し、Ａはカルシウム（Ｃａ）、ストロンチウム（Ｓｒ）、バリウム（Ｂａ）、亜鉛（Ｚｎ）、またはこれらの混合物である。）
［４９］［１８］〜［３１］のいずれかに記載の発光装置であって、発光要素として半導体発光素子と蛍光体を備え、前記半導体発光素子は発光スペクトルのピーク波長が３９５ｎｍ以上４２０ｎｍ未満であり、前記蛍光体は、ＳＢＣＡ、β−ＳｉＡｌＯＮ、およびＣＡＳＯＮを含むことを特徴とする発光装置。
［５０］［１８］〜［３１］のいずれかに記載の発光装置であって、発光要素として半導体発光素子と蛍光体を備え、前記半導体発光素子は発光スペクトルのピーク波長が３９５ｎｍ以上４２０ｎｍ未満であり、前記蛍光体は、ＳＣＡ、β−ＳｉＡｌＯＮ、およびＣＡＳＯＮを含むことを特徴とする発光装置。
［５１］［１８］〜［５０］のいずれかに記載の発光装置であって、パッケージ化ＬＥＤ、ＬＥＤモジュール、ＬＥＤ照明器具、およびＬＥＤ照明システムからなる群から選択されるいずれかであることを特徴とする発光装置。
［５２］家庭用照明装置として用いられる、［１８］〜［５１］のいずれかに記載の発光装置。
［５３］展示物用照明装置として用いられる、［１８］〜［５１］のいずれかに記載の発光装置。
［５４］演出用照明装置として用いられる、［１８］〜［５１］のいずれかに記載の発光装置。
［５５］医療用照明装置として用いられる、［１８］〜［５１］のいずれかに記載の発光装置。［５６］作業用照明装置として用いられる、［１８］〜［５１］のいずれかに記載の発光装置。
［５７］工業機器内用照明装置として用いられる、［１８］〜［５１］のいずれかに記載の発光装置。
［５８］交通機関内装用照明装置として用いられる、［１８］〜［５１］のいずれかに記載の発光装置。
［５９］美術品用照明装置として用いられる、［１８］〜［５１］のいずれかに記載の発光装置。
［６０］高齢者用照明装置として用いられる、［１８］〜［５１］のいずれかに記載の発光装置。

上記目的を達成するため、本発明の第二の実施態様は以下の事項に関する。
［６１］発光要素と制御要素とを内在する発光装置の設計方法であって、波長をλ（ｎｍ）とし、
当該発光要素から出射される全放射束分光分布をΦ_ｅｌｍ（λ）、定義された波長範囲内の最大全放射束分光強度Φ_{ｅｌｍｍａｘ}を与える波長λをλ_{ｅｌｍｍａｘ}（ｎｍ）、Φ_ｅｌｍ（λ）をΦ_{ｅｌｍｍａｘ}で除した発光要素の相対全放射束分光分布をΦ_{ｅｌｍｒｅｌ}（λ）とし、
当該発光装置から主たる放射方向に出射される光の分光分布をφ_ＳＳＬ（λ）、φ_ＳＳＬ（λ）をφ_ＳＳＬ（λ_{ｅｌｍｍａｘ}）で除した発光装置の相対分光分布をφ_{ＳＳＬｒｅｌ}（λ）とした際に、
当該制御要素によってΦ_{ｅｌｍｒｅｌ}（λ）で表される光とφ_{ＳＳＬｒｅｌ}（λ）で表される光が条件１および条件２をいずれも満たし、かつ、φ_{ＳＳＬｒｅｌ}（λ）で表される光が条件３を満たすことを特徴とする発行装置の設計方法。
＜条件１＞
５３０ｎｍ≦λ≦５８０ｎｍの全λにおいて
０．７０ ≦φ_{ＳＳＬｒｅｌ}（λ）／Φ_{ｅｌｍｒｅｌ}（λ）≦ １．３０が成立する。
＜条件２＞
３８０ｎｍ≦λ≦７８０ｎｍにおいて、
φ_{ＳＳＬｒｅｌ}（λ）／Φ_{ｅｌｍｒｅｌ}（λ）≦０．９７ または １．０３≦φ_{ＳＳＬｒｅｌ}（λ）／Φ_{ｅｌｍｒｅｌ}（λ）を満たすλが存在する。
＜条件３＞
３８０ｎｍ≦λ≦７８０ｎｍにおいて、
φ_{ＳＳＬｒｅｌ}（λ）に係る、ＡＮＳＩ Ｃ７８．３７７で定義される黒体放射軌跡からの距離Ｄ_uvSSLが、−０．０３５０ ≦ Ｄ_uvSSL ≦ −０．００４０である。

上記目的を達成するため、本発明の第三の実施態様は以下の事項に関する。
［６２］発光要素と制御要素とを内在する発光装置から出射される光により対象物を照明する照明工程、を含む照明方法であって、
波長をλ（ｎｍ）とし、
当該発光要素から出射される全放射束分光分布をΦ_ｅｌｍ（λ）、定義された波長範囲内の最大全放射束分光強度Φ_{ｅｌｍｍａｘ}を与える波長λをλ_{ｅｌｍｍａｘ}（ｎｍ）、Φ_ｅｌｍ（λ）をΦ_{ｅｌｍｍａｘ}で除した発光要素の相対全放射束分光分布をΦ_{ｅｌｍｒｅｌ}（λ）とし、
当該発光装置から主たる放射方向に出射される光の分光分布をφ_ＳＳＬ（λ）、φ_ＳＳＬ（λ）をφ_ＳＳＬ（λ_{ｅｌｍｍａｘ}）で除した発光装置の相対分光分布をφ_{ＳＳＬｒｅｌ}（λ）とした際に、
当該制御要素によってΦ_{ｅｌｍｒｅｌ}（λ）で表される光とφ_{ＳＳＬｒｅｌ}（λ）で表される光が条件１および条件２をいずれも満たし、かつ、φ_{ＳＳＬｒｅｌ}（λ）で表される光が条件３を満たすことを特徴とする発光装置から出射される光により対象物を照明する照明工程、を含む照明方法。
＜条件１＞
５３０ｎｍ≦λ≦５８０ｎｍの全λにおいて
０．７０ ≦φ_{ＳＳＬｒｅｌ}（λ）／Φ_{ｅｌｍｒｅｌ}（λ）≦ １．３０が成立する。
＜条件２＞
３８０ｎｍ≦λ≦７８０ｎｍにおいて、
φ_{ＳＳＬｒｅｌ}（λ）／Φ_{ｅｌｍｒｅｌ}（λ）≦０．９７ または １．０３≦φ_{ＳＳＬｒｅｌ}（λ）／Φ_{ｅｌｍｒｅｌ}（λ）を満たすλが存在する。
＜条件３＞
３８０ｎｍ≦λ≦７８０ｎｍにおいて、
φ_{ＳＳＬｒｅｌ}（λ）に係る、ＡＮＳＩ Ｃ７８．３７７で定義される黒体放射軌跡からの距離Ｄ_uvSSLが、−０．０３５０ ≦ Ｄ_uvSSL ≦ −０．００４０である。 In order to achieve the above object, the first embodiment of the present invention relates to the following items.
[1] A light emitting device including a light emitting element and a control element,
Let the wavelength be λ (nm),
The total radiant flux spectral distribution emitted from the light emitting element is Φ _elm (λ), and the wavelength λ giving the maximum total radiant flux spectral intensity Φ _elmmax within the defined wavelength range is λ _elmmax (nm), Φ _elm (λ) _Is the relative total radiant flux spectral distribution of the light-emitting element divided by Φ _elmmax , and Φ _elmrel (λ),
The relative spectral distribution of the light emitting device obtained by dividing the spectral distribution of the light emitted from the light emitting device in the main radiation direction by φ _SSL (λ) and φ _SSL (λ) by φ _SSL (λ _elmmax ) is φ _SSLrel (λ). When
The light expressed by Φ _elmrel (λ) and the light expressed by φ _SSLrel (λ) satisfy both the conditions 1 and 2 by the control element, and the light expressed by φ _SSLrel (λ) is a condition. 3, a light emitting device satisfying the above requirement.
<Condition 1>
In all λ of 530 nm ≦ λ ≦ 580 nm, 0.70 ≦ φ _SSLrel (λ) / Φ _elmrel (λ) ≦ 1.30 holds.
<Condition 2>
At 380 nm ≦ λ ≦ 780 nm,
There _exists λ _satisfying φ _SSLrel (λ) / Φ _elmrel (λ) ≦ 0.97 or 1.03 ≦ φ _SSLrel (λ) / Φ _elmrel (λ).
<Condition 3>
At 380 nm ≦ λ ≦ 780 nm,
The distance D _uvSSL from the black body radiation locus defined by ANSI C78.377 related to φ _SSLrel (λ) is −0.0350 ≦ D _uvSSL ≦ −0.0040.
[2] The light emitting device according to [1], wherein the light emitting device also satisfies condition 4. <Condition 4>
0.90 ≦ φ _SSLrel (λ) / Φ _elmrel (λ) ≦ 1.10 holds for all λ of 530 nm ≦ λ ≦ 580 nm.
[3] A light-emitting device according to [1] or [2], wherein the light-emitting device also satisfies condition 5.
<Condition 5>
0.80 ≦ φ _SSLrel (λ) / Φ _elmrel (λ) ≦ 1.20 holds for all λ of 495 nm ≦ λ ≦ 590 nm.
[4] A light-emitting device according to any one of [1] to [3], wherein the light-emitting device also satisfies condition 6.
<Condition 6>
At 380 nm ≦ λ ≦ 495 nm,
There _exists λ _satisfying φ _SSLrel (λ) / Φ _elmrel (λ) ≦ 0.70 or 1.30 ≦ φ _SSLrel (λ) / Φ _elmrel (λ).
[5] The light emitting device according to [4], wherein the light emitting device also satisfies condition 7. <Condition 7>
At 380 nm ≦ λ ≦ 495 nm,
There _exists λ _satisfying φ _SSLrel (λ) / Φ _elmrel (λ) ≦ 0.40 or 1.60 ≦ φ _SSLrel (λ) / Φ _elmrel (λ).
[6] The light-emitting device according to [4] or [5], wherein the light-emitting device also satisfies condition 8.
<Condition 8>
At 380 nm ≦ λ ≦ 495 nm,
There _exists λ _satisfying φ _SSLrel (λ) / Φ _elmrel (λ) ≦ 0.10 or 1.90 ≦ φ _SSLrel (λ) / Φ _elmrel (λ).
[7] The light emitting device according to any one of [1] to [6], wherein the light emitting device also satisfies condition 9.
<Condition 9>
At 590 nm ≦ λ ≦ 780 nm,
There _exists λ _satisfying φ _SSLrel (λ) / Φ _elmrel (λ) ≦ 0.70 or 1.30 ≦ φ _SSLrel (λ) / Φ _elmrel (λ).
[8] The light-emitting device according to [7], wherein the light-emitting device also satisfies the condition 10.
<Condition 10>
At 590 nm ≦ λ ≦ 780 nm,
There _exists λ _satisfying φ _SSLrel (λ) / Φ _elmrel (λ) ≦ 0.40 or 1.60 ≦ φ _SSLrel (λ) / Φ _elmrel (λ).
[9] A light-emitting device according to [7] or [8], which also satisfies the condition 11.
<Condition 11>
At 590 nm ≦ λ ≦ 780 nm,
There _exists λ _satisfying φ _SSLrel (λ) / Φ _elmrel (λ) ≦ 0.10 or 1.90 ≦ φ _SSLrel (λ) / Φ _elmrel (λ).
[10] The light-emitting device according to any one of [1] to [9], wherein the control element absorbs or reflects light in a λ (nm) ≦ 450 nm region.
[11] The light emitting device according to [10], wherein the control element absorbs or reflects light in a λ (nm) ≦ 410 nm region in a direction different from a main radiation direction of the light emitting device. apparatus.
[12] The light-emitting device according to any one of [1] to [11], wherein the control element absorbs light in a region of 710 nm ≦ λ (nm) or reflects in a direction different from a main radiation direction of the light-emitting device. A light emitting device characterized by:
[13] The light-emitting device according to [12], wherein the control element absorbs or reflects light in a region of 750 nm ≦ λ (nm).
[14] The light-emitting device according to any one of [1] to [13], wherein the control element has a function of condensing and / or diffusing light emitted from the light-emitting element. Light emitting device.
[15] The light-emitting device according to [14], wherein the light condensing and / or diffusing function of the control element is realized by at least one function of a concave lens, a convex lens, and a Fresnel lens.
[16] The light emitting device according to any one of [1] to [15], wherein the light emitting element includes a semiconductor light emitting element.
[17] The light-emitting device according to any one of [1] to [16], which is defined by ANSI C78.377 relating to a total radiant flux spectral distribution Φ _elm (λ) emitted from the light-emitting element. A light emitting device, wherein a distance D _uvelm from a black body radiation locus is −0.0350 ≦ D _uvelm ≦ −0.0040.
[18] The light-emitting device according to any one of [1] to [17],

The reference light spectral distribution selected according to the correlated color temperature T _SSL (K) of the light derived from φ _SSL (λ) is φ _ref (λ), and is emitted from the light emitting device in the radiation direction. The tristimulus values of light (X _SSL , Y _SSL , Z _SSL ) and the reference tristimulus values of light selected according to T _SSL (K) of light emitted from the light emitting device in the radiation direction ( X _ref , Y _ref , Z _ref )
A standard selected according to the normalized spectral distribution S _SSL (λ) of light emitted from the light emitting device in the emission direction and T _SSL (K) of light emitted from the light emission device in the emission direction. The normalized spectral distribution S _ref (λ) of light and the difference ΔS (λ) between these normalized spectral distributions are respectively
S _SSL (λ) = φ _SSL (λ) / Y _SSL
S _ref (λ) = φ _ref (λ) / Y _ref
ΔS (λ) = S _ref (λ) −S _SSL (λ)
And define
Within a range of wavelength 380nm or 780 _nm, the wavelength giving the longest wavelength maximum of the _{S SSL} (lambda) upon the _{λ R (nm), λ S} SSL (λ R) on the longer wavelength side than _R / 2 and There exists a wavelength Λ4,
An index A _cg represented by the following mathematical formula (1) satisfies −360 ≦ A _cg ≦ −10.

[19] The light-emitting device according to any one of [1] to [17],
The reference light spectral distribution selected according to the correlated color temperature T _SSL (K) of the light derived from φ _SSL (λ) is φ _ref (λ), and is emitted from the light emitting device in the radiation direction. The tristimulus values of light (X _SSL , Y _SSL , Z _SSL ) and the reference tristimulus values of light selected according to T _SSL (K) of light emitted from the light emitting device in the radiation direction ( X _ref , Y _ref , Z _ref )
A standard selected according to the normalized spectral distribution S _SSL (λ) of light emitted from the light emitting device in the emission direction and T _SSL (K) of light emitted from the light emission device in the emission direction. The normalized spectral distribution S _ref (λ) of light and the difference ΔS (λ) between these normalized spectral distributions are respectively
S _SSL (λ) = φ _SSL (λ) / Y _SSL
S _ref (λ) = φ _ref (λ) / Y _ref
ΔS (λ) = S _ref (λ) −S _SSL (λ)
And define
Within a range of wavelength 380nm or 780 _nm, the wavelength giving the longest wavelength maximum of the _{S SSL} (lambda) upon the _{λ R (nm), λ S} SSL (λ R) on the longer wavelength side than _R / 2 and There is no wavelength Λ4,
An index A _cg represented by the following mathematical formula (2) satisfies −360 ≦ A _cg ≦ −10.

[20] The light-emitting device according to [18] or [19],
The light emitted from the light emitting device in the radiation direction satisfies the following (1) and (2).
(1) CIE 1976 L ^* a ^* b ^{* of the following} 15 modified Munsell color charts from # 01 to # 15 when mathematically assuming illumination by light emitted in the radiation direction from the light emitting device
The a ^* value and b ^* value in the color space are a ^* _nSSL and b ^* _nSSL (where n is a natural number from 1 to 15, respectively)
CIE 1976 of the 15 kinds of modified Munsell color charts when the illumination with the reference light selected according to the correlated color temperature T _SSL (K) of the light emitted in the radiation direction is mathematically assumed.
When the a ^* value and b ^* value in the L ^* a ^* b ^* color space are a ^* _nref and b ^* _nref (where n is a natural number from 1 to 15), the saturation difference ΔC _n is −3.8. ≦ ΔC _n ≦ 18.6 (n is a natural number from 1 to 15)
And the average saturation difference represented by the following formula (3) satisfies the following formula (4):

When the maximum value of the saturation difference is ΔC _max and the minimum value of the saturation difference is ΔC _min , the difference ΔC _max −ΔC _min between the maximum value of the saturation difference and the minimum value of the saturation difference is 2.8 ≦ (ΔC _max −ΔC _min ) ≦ 19.6
Meet.
Note that ΔC _n = √ {(a ^* _nSSL ) ² + (b ^* _nSSL ) ² } −√ {(a ^* _nref ) ² + (b ^* _nref ) ² }.
15 types of modified Munsell color chart # 01 7.5 P 4/10
# 02 10 PB 4/10
# 03 5 PB 4/12
# 04 7.5 B 5/10
# 05 10 BG 6/8
# 06 2.5 BG 6/10
# 07 2.5 G 6/12
# 08 7.5 GY 7/10
# 09 2.5 GY 8/10
# 10 5 Y 8.5 / 12
# 11 10 YR 7/12
# 12 5 YR 7/12
# 13 10 R 6/12
# 14 5 R 4/14
# 15 7.5 RP 4/12
(2) The hue angle in the CIE 1976 L ^* a ^* b ^* color space of the above 15 types of modified Munsell color _charts when the illumination by the light emitted from the light emitting device in the radiation direction is mathematically assumed is θ _nSSL. (Degree) (where n is a natural number from 1 to 15)
CIE 1976 of the 15 kinds of modified Munsell color charts when the illumination with the reference light selected according to the correlated color temperature T _SSL (K) of the light emitted in the radiation direction is mathematically assumed.
When the hue angle in the L ^* a ^* b ^* color space is θ _nref (degrees) (where n is a natural number from 1 to 15), the absolute value of the hue angle difference | Δh _n | is 0 ≦ | Δh _n | ≦ 9.0 (degrees) (n is a natural number from 1 to 15)
Meet.
However, it is set as _{( DELTA) hn} = (theta) _{nSSL- (} theta) _nref .
[21] The light-emitting device according to any one of [18] to [20],
The light emitted from the light emitting device in the radiation direction has a radiation efficiency K (lm / W) in the range of 380 nm to 780 nm derived from the spectral distribution φ _SSL (λ), 180 (lm / W) ≦ K (Lm / W) ≦ 320 (lm / W)
A light emitting device characterized by satisfying the above.
[22] The light-emitting device according to [20], wherein the absolute value | Δh _n | of the hue angle difference is 0.0003 ≦ | Δh _n | ≦ 8.3 (degrees) (n is a natural number of 1 to 15) )
A light emitting device characterized by satisfying the above.
[23] The light-emitting device according to [20], wherein the average saturation difference represented by the general formula (3) satisfies the following formula (4) ′.

(4) '
[24] The light emitting device according to [20], wherein the saturation difference ΔC _n is −3.4 ≦ ΔC _n ≦ 16.8 (n is a natural number from 1 to 15).
A light emitting device characterized by satisfying the above.
[25] The light-emitting device according to [20], wherein a difference ΔC _max −ΔC _min between the maximum value of the saturation difference and the minimum value of the saturation difference is 3.2 ≦ (ΔC _max − ΔC _min ) ≦ 17.8
A light emitting device characterized by satisfying the above.
[26] The light-emitting device according to any one of [18] to [25],
The light emitted from the light emitting device in the radiation direction has a distance D _uvSSL from the black body radiation locus of −0.0250 ≦ D _uvSSL ≦ −0.0100.
A light emitting device characterized by satisfying the above.
[27] The light-emitting device according to any one of [18] to [26], wherein the index A _cg represented by the formula (1) or (2) is −322 ≦ A _cg ≦ −12.
A light emitting device characterized by satisfying the above.
[28] The light-emitting device according to any one of [18] to [27],
The light emitted from the light emitting device in the radiation direction has a radiation efficiency K (lm / W) in a wavelength range of 380 nm or more and 780 nm or less derived from the spectral distribution φ _SSL (λ).
206 (lm / W) ≦ K (lm / W) ≦ 288 (lm / W)
A light emitting device characterized by satisfying the above.
[29] The light-emitting device according to any one of [18] to [28], wherein the correlated color temperature T _SSL (K) is 2550 (K) ≦ T _SSL (K) ≦ 5650 (K).
A light emitting device characterized by satisfying the above.
[30] The light-emitting device according to any one of [18] to [29], wherein an illuminance at which light emitted from the light-emitting device in the radiation direction illuminates an object is 150 lx or more and 5000 lx or less. A light emitting device characterized.
[31] The light-emitting device according to any one of [18] to [30], wherein the light-emitting device emits light emitted from one to six types of light-emitting elements in the radiation direction. Light-emitting device.
[32] The light emitting device according to any one of [18] to [31], wherein the light emitting device includes a semiconductor light emitting element as a light emitting element, and a peak wavelength of an emission spectrum of the semiconductor light emitting element is 380 nm or more and less than 495 nm. And a full width at half maximum of 2 nm to 45 nm.
[33] The light-emitting device according to [32], wherein a peak wavelength of an emission spectrum of the semiconductor light-emitting element is 395 nm or more and less than 420 nm.
[34] The light-emitting device according to [32], wherein a peak wavelength of an emission spectrum of the semiconductor light-emitting element is 420 nm or more and less than 455 nm.
[35] The light-emitting device according to [32], wherein a peak wavelength of an emission spectrum of the semiconductor light-emitting element is not less than 455 nm and less than 485 nm.
[36] The light emitting device according to any one of [18] to [31], wherein the light emitting device includes a semiconductor light emitting element as a light emitting element, and a peak wavelength of an emission spectrum of the semiconductor light emitting element is not less than 495 nm and less than 590 nm. And a full width at half maximum of 2 nm to 75 nm.
[37] The light emitting device according to any one of [18] to [31], wherein the light emitting device includes a semiconductor light emitting element as a light emitting element, and a peak wavelength of an emission spectrum of the semiconductor light emitting element is not less than 590 nm and less than 780 nm. And a full width at half maximum of 2 nm to 30 nm.
[38] The light emitting device according to any one of [18] to [31], wherein the light emitting device includes a semiconductor light emitting element as a light emitting element, and the semiconductor light emitting element is a sapphire substrate, a GaN substrate, a GaAs substrate, GaP. A light emitting device produced on any substrate selected from the group consisting of substrates.
[39] The light emitting device according to any one of [18] to [31], wherein the light emitting device includes a semiconductor light emitting element as a light emitting element, and the semiconductor light emitting element is formed on a GaN substrate or a GaP substrate. And the thickness of the said board | substrate is 100 micrometers or more and 2 mm or less, The light-emitting device characterized by the above-mentioned.
[40] The light emitting device according to any one of [18] to [32], wherein the light emitting device includes a semiconductor light emitting element as a light emitting element, and the semiconductor light emitting element is formed on a sapphire substrate or a GaAs substrate. The light emitting device is characterized in that the semiconductor light emitting element is peeled off from the substrate.
[41] The light-emitting device according to any one of [18] to [35], comprising a phosphor as a light-emitting element.
[42] The light-emitting device according to [41], wherein the phosphor includes one to five phosphors having different emission spectra.
[43] The light-emitting device according to [41] or [42], wherein the phosphor has a peak wavelength of a single emission spectrum of 380 nm or more and less than 495 nm when photoexcited at room temperature, and has a full width at half maximum. A light emitting device comprising a phosphor having a thickness of 2 nm to 90 nm.
[44] The light-emitting device according to [43], wherein the phosphor is represented by the following general formula (5), the phosphor represented by the following general formula (5) ', (Sr, Ba ) ₃ MgSi ₂ O ₈ : Eu ²⁺ , and (Ba, Sr, Ca, Mg) Si ₂ O ₂ N ₂ : Eu includes at least one selected from the group consisting of Eu.
(Ba, Sr, Ca) MgAl ₁₀ O ₁₇ : Mn, Eu (5)
_{Sr a Ba b Eu x (PO} 4) c X d (5) '
(In the general formula (5) ′, X is Cl. Also, c, d and x are 2.7 ≦ c ≦ 3.3, 0.9 ≦ d ≦ 1.1, 0.3 ≦ x ≦. (In addition, a and b satisfy the condition of a + b = 5-x and 0 ≦ b / (a + b) ≦ 0.6.)
[45] The light-emitting device according to [41] or [42], wherein the phosphor has a peak wavelength of a single emission spectrum of 495 nm or more and less than 590 nm when photoexcited at room temperature, and has a full width at half maximum. A light-emitting device including a phosphor with a thickness of 2 nm to 130 nm.
[46] The light emitting device according to [45], wherein the phosphor is Si _6-z Al _z O _z N _8-z : Eu (where 0 <z <4.2), and the following general formula (6): in phosphor represented, phosphor represented by the following general formula (6) ', and SrGaS _4: light-emitting device which comprises at least one selected from the group consisting of Eu ^2+.
_{(Ba a Ca b Sr c Mg} d Eu x) SiO 4 (6)
(In the general formula (6), a, b, c, d and x are a + b + c + d + x = 2, 1.0 ≦ a ≦ 2.0, 0 ≦ b <0.2, 0.2 ≦ c ≦ 0.8, 0 ≦ d <0.2
And 0 <x ≦ 0.5. )
Ba _1-xy Sr _x Eu _y Mg _1-z Mn _z Al ₁₀ O ₁₇ (6) ′
(In the general formula (6) ′, x, y, and z satisfy 0.1 ≦ x ≦ 0.4, 0.25 ≦ y ≦ 0.6, and 0.05 ≦ z ≦ 0.5, respectively.)
[47] The light-emitting device according to [41] or [42], wherein the phosphor has a peak wavelength of a single emission spectrum of 590 nm or more and less than 780 nm when photoexcited at room temperature, and has a full width at half maximum A light-emitting device including a phosphor with a thickness of 2 nm to 130 nm.
[48] The light-emitting device according to [47], wherein the phosphor is represented by the following general formula (7), the phosphor represented by the following general formula (7) ', (Sr, Ca _{, Ba) 2 Al x Si 5} -x O x N 8-x: Eu ( provided that _{0 ≦ x ≦ 2), Eu} y (Sr, Ca, Ba) 1-y: Al 1 + x Si 4-x O x N 7 _-x (except _{0 ≦ x <4,0 ≦ y <} 0.2), K 2 SiF 6: Mn 4+, A 2 + x M y Mn z F n (A is Na and / or K; M is Si and Al; −1 ≦ x ≦ 1 and 0.9 ≦ y + z ≦ 1.1 and 0.001 ≦ z ≦ 0.4 and 5 ≦ n ≦ 7), (Ca, Sr, Ba, Mg) AlSiN ₃ : Eu and / or (Ca, Sr, Ba) AlSiN ₃ : Eu, and (CaAlSiN ₃ ) _1-x (Si ₂ N ₂ O) _x : E A light emitting device including one or more selected from the group consisting of u (where x is 0 <x <0.5).
_{(La 1-x-y,} Eu x, Ln y) 2 O 2 S (7)
(In the general formula (7), x and y represent numbers satisfying 0.02 ≦ x ≦ 0.50 and 0 ≦ y ≦ 0.50, respectively, and Ln represents Y, Gd, Lu, Sc, Sm and Er. Represents at least one trivalent rare earth element)
(K−x) MgO.xAF ₂ .GeO ₂ : yMn ⁴⁺ (7) ′
(In general formula (7) ′, k, x, and y represent numbers satisfying 2.8 ≦ k ≦ 5, 0.1 ≦ x ≦ 0.7, and 0.005 ≦ y ≦ 0.015, respectively. , A is calcium (Ca), strontium (Sr), barium (Ba), zinc (Zn), or a mixture thereof.
[49] The light-emitting device according to any one of [18] to [31], wherein the light-emitting element includes a semiconductor light-emitting element and a phosphor, and the semiconductor light-emitting element has an emission spectrum peak wavelength of 395 nm or more and less than 420 nm. And the phosphor includes SBCA, β-SiAlON, and CASON.
[50] The light-emitting device according to any one of [18] to [31], comprising a semiconductor light-emitting element and a phosphor as light-emitting elements, wherein the semiconductor light-emitting element has an emission spectrum peak wavelength of 395 nm or more and less than 420 nm. And the phosphor includes SCA, β-SiAlON, and CASON.
[51] The light-emitting device according to any one of [18] to [50], which is any one selected from the group consisting of packaged LEDs, LED modules, LED lighting fixtures, and LED lighting systems. A light emitting device characterized.
[52] The light-emitting device according to any one of [18] to [51], which is used as a home lighting device.
[53] The light-emitting device according to any one of [18] to [51], which is used as an illumination device for an exhibit.
[54] The light-emitting device according to any one of [18] to [51], which is used as an effect lighting device.
[55] The light-emitting device according to any one of [18] to [51], which is used as a medical lighting device. [56] The light-emitting device according to any one of [18] to [51], which is used as a work lighting device.
[57] The light-emitting device according to any one of [18] to [51], which is used as a lighting device for industrial equipment.
[58] The light-emitting device according to any one of [18] to [51], which is used as a lighting device for transportation interiors.
[59] The light-emitting device according to any one of [18] to [51], which is used as a lighting device for art.
[60] The light-emitting device according to any one of [18] to [51], which is used as an illumination device for elderly people.

In order to achieve the above object, the second embodiment of the present invention relates to the following items.
[61] A method of designing a light emitting device including a light emitting element and a control element, wherein the wavelength is λ (nm),
The total radiant flux spectral distribution emitted from the light emitting element is Φ _elm (λ), and the wavelength λ giving the maximum total radiant flux spectral intensity Φ _elmmax within the defined wavelength range is λ _elmmax (nm), Φ _elm (λ) _Is the relative total radiant flux spectral distribution of the light-emitting element divided by Φ _elmmax , and Φ _elmrel (λ),
The relative spectral distribution of the light emitting device obtained by dividing the spectral distribution of the light emitted from the light emitting device in the main radiation direction by φ _SSL (λ) and φ _SSL (λ) by φ _SSL (λ _elmmax ) is φ _SSLrel (λ). When
The light expressed by Φ _elmrel (λ) and the light expressed by φ _SSLrel (λ) satisfy both the conditions 1 and 2 by the control element, and the light expressed by φ _SSLrel (λ) is a condition. 3 is a method for designing an issuing apparatus.
<Condition 1>
In all λ of 530 nm ≦ λ ≦ 580 nm, 0.70 ≦ φ _SSLrel (λ) / Φ _elmrel (λ) ≦ 1.30 holds.
<Condition 2>
At 380 nm ≦ λ ≦ 780 nm,
There _exists λ _satisfying φ _SSLrel (λ) / Φ _elmrel (λ) ≦ 0.97 or 1.03 ≦ φ _SSLrel (λ) / Φ _elmrel (λ).
<Condition 3>
At 380 nm ≦ λ ≦ 780 nm,
The distance D _uvSSL from the black body radiation locus defined by ANSI C78.377 related to φ _SSLrel (λ) is −0.0350 ≦ D _uvSSL ≦ −0.0040.

In order to achieve the above object, the third embodiment of the present invention relates to the following items.
[62] An illumination method including an illumination step of illuminating an object with light emitted from a light emitting device including a light emitting element and a control element,
Let the wavelength be λ (nm),
The total radiant flux spectral distribution emitted from the light emitting element is Φ _elm (λ), and the wavelength λ giving the maximum total radiant flux spectral intensity Φ _elmmax within the defined wavelength range is λ _elmmax (nm), Φ _elm (λ) _Is the relative total radiant flux spectral distribution of the light-emitting element divided by Φ _elmmax , and Φ _elmrel (λ),
The relative spectral distribution of the light emitting device obtained by dividing the spectral distribution of the light emitted from the light emitting device in the main radiation direction by φ _SSL (λ) and φ _SSL (λ) by φ _SSL (λ _elmmax ) is φ _SSLrel (λ). When
The light expressed by Φ _elmrel (λ) and the light expressed by φ _SSLrel (λ) satisfy both the conditions 1 and 2 by the control element, and the light expressed by φ _SSLrel (λ) is a condition. 3. An illumination method including an illumination step of illuminating an object with light emitted from the light emitting device satisfying 3.
<Condition 1>
In all λ of 530 nm ≦ λ ≦ 580 nm, 0.70 ≦ φ _SSLrel (λ) / Φ _elmrel (λ) ≦ 1.30 holds.
<Condition 2>
At 380 nm ≦ λ ≦ 780 nm,
There _exists λ _satisfying φ _SSLrel (λ) / Φ _elmrel (λ) ≦ 0.97 or 1.03 ≦ φ _SSLrel (λ) / Φ _elmrel (λ).
<Condition 3>
At 380 nm ≦ λ ≦ 780 nm,
The distance D _uvSSL from the black body radiation locus defined by ANSI C78.377 related to φ _SSLrel (λ) is −0.0350 ≦ D _uvSSL ≦ −0.0040.

According to the present invention, and when illuminated with (if there is described a laboratory reference light) reference light and a high R _a and high R _i becomes color appearance close to the light of the reference light Compared to the case of illuminating with a light emitting device that emits (which may be described as a pseudo-reference light for experiments), a large number of subjects are statistically more likely to have a similar CCT and substantially the same illuminance. A light-emitting device and illumination method capable of realizing the appearance of a truly good object color that is judged to be good can be realized, and a light-emitting device and illumination method capable of reducing the degree of optical alteration of an illumination object are realized. Is done.

More specifically, the effects realized by the present invention are as follows.
First, when illuminated with a light-emitting device such as a light source, instrument, system, etc. according to the present invention, or when illuminated with the illumination method of the present invention, illuminated with experimental reference light or experimental pseudo-reference light, etc. In contrast, even with almost the same CCT and almost the same illuminance, white is whiter and looks natural and comfortable. Furthermore, it becomes easy to visually recognize the brightness difference between achromatic colors such as white, gray, and black. For this reason, for example, black characters on general white paper are easy to read. Although details will be described later, such an effect is completely unexpected in light of conventional common sense.
Second, the illuminance realized by the light emitting device according to the present invention or the illuminance when illuminated by the illumination method of the present invention is purple even if the ordinary indoor environment is about several thousand Lx to several hundred Lx. , Violet, blue, blue-green, green, yellow-green, yellow, yellow-red, red, red-purple, etc. A truly natural color appearance as seen below about lx is achieved. In addition, the skin color of subjects (Japanese people), various foods, clothing, wood colors, and the like, which have intermediate saturation, have natural colors that many subjects feel more preferable.
Third, when illuminated with the light emitting device according to the present invention even when the illumination is substantially the same CCT and substantially the same illuminance as compared with the illumination with the experimental reference light or the experimental pseudo-reference light, or When illuminated by the illumination method of the present invention, it is easy to identify colors in adjacent hues, and it is possible to perform comfortable work as if in a high illumination environment. More specifically, for example, a plurality of lipsticks having similar red colors can be more easily identified.
Fourth, when illuminated with the light source, instrument, or system according to the present invention even when the illumination is substantially the same CCT and substantially the same illuminance as compared with the illumination with the experimental reference light or the experimental reference light, etc. Or, when illuminated by the illumination method of the present invention, the object can be seen more clearly and easily as if viewed in a high-illuminance environment.
Furthermore, in the present invention, by reducing the relative spectral intensity of ultraviolet light, near ultraviolet light, violet light, etc. that can be emitted from the light emitting device and applied to the illumination object, and / or near infrared, infrared, By reducing the relative spectral intensity of far-infrared light or the like, the first to fourth effects can be realized while reducing the degree of optical alteration to the illumination object.

Built-in semiconductor light emitting device with a peak wavelength of 459 nm, emitted from a package LED having a green phosphor and a red phosphor, and a spectral distribution assumed to illuminate 15 kinds of modified Munsell color charts, and illuminated by the LED And CIELAB color space in which a ^* values and b ^* values of the fifteen types of modified Munsell color charts when illuminated with reference light are plotted. A semiconductor light emitting device having a peak wavelength of 475 nm is incorporated, and is emitted from a package LED including a green phosphor and a red phosphor. And CIELAB color space in which a ^* values and b ^* values of the fifteen kinds of corrected Munsell color charts when illuminated with reference light are plotted together. A semiconductor light-emitting device having a peak wavelength of 425 nm is embedded, and is emitted from a package LED including a green phosphor and a red phosphor, and a spectral distribution that is assumed to illuminate 15 types of modified Munsell color charts. And CIELAB color space in which a ^* values and b ^* values of the fifteen types of modified Munsell color charts when illuminated with reference light are plotted. Built-in semiconductor light emitting device with a peak wavelength of 459 nm, emitted from a package LED having a green phosphor and a red phosphor, and a spectral distribution assumed to illuminate 15 kinds of modified Munsell color charts, and illuminated by the LED And CIELAB color space in which a ^* values and b ^* values of the 15 types of modified Munsell color charts when illuminated with reference light are plotted (Duv = 0.0000). Built-in semiconductor light emitting device with a peak wavelength of 459 nm, emitted from a package LED having a green phosphor and a red phosphor, and a spectral distribution assumed to illuminate 15 kinds of modified Munsell color charts, and illuminated by the LED And CIELAB color space in which a ^* values and b ^* values of the 15 types of modified Munsell color charts when illuminated with reference light are plotted (Duv = 0.0100). Built-in semiconductor light emitting device with a peak wavelength of 459 nm, emitted from a package LED having a green phosphor and a red phosphor, and a spectral distribution assumed to illuminate 15 kinds of modified Munsell color charts, and illuminated by the LED And CIELAB color space in which the a ^* value and b ^* value of the 15 types of modified Munsell color charts when illuminated with reference light are plotted (Duv = 0.150). Built-in semiconductor light emitting device with a peak wavelength of 459 nm, emitted from a package LED having a green phosphor and a red phosphor, and a spectral distribution assumed to illuminate 15 kinds of modified Munsell color charts, and illuminated by the LED And CIELAB color space in which a ^* values and b ^* values of the 15 types of modified Munsell color charts when illuminated with reference light are plotted (Duv = −0.0100). Built-in semiconductor light emitting device with a peak wavelength of 459 nm, emitted from a package LED having a green phosphor and a red phosphor, and a spectral distribution assumed to illuminate 15 kinds of modified Munsell color charts, and illuminated by the LED And CIELAB color space in which the a ^* value and b ^* value of the 15 types of modified Munsell color charts when illuminated with reference light are plotted (Duv = −0.0200). Built-in semiconductor light emitting device with a peak wavelength of 459 nm, emitted from a package LED having a green phosphor and a red phosphor, and a spectral distribution assumed to illuminate 15 kinds of modified Munsell color charts, and illuminated by the LED And CIELAB color space in which the a ^* value and b ^* value of the 15 types of modified Munsell color charts when illuminated with reference light are plotted (Duv = −0.0300). Built-in semiconductor light emitting device with a peak wavelength of 459 nm, emitted from a package LED having a green phosphor and a red phosphor, and a spectral distribution assumed to illuminate 15 kinds of modified Munsell color charts, and illuminated by the LED And CIELAB color space in which a ^* values and b ^* values of the 15 types of corrected Munsell color charts when illuminated with reference light are plotted (Duv = −0.0400). Built-in semiconductor light emitting device with a peak wavelength of 459 nm, emitted from a package LED having a green phosphor and a red phosphor, and a spectral distribution assumed to illuminate 15 kinds of modified Munsell color charts, and illuminated by the LED And CIELAB color space in which a ^* values and b ^* values of the fifteen types of modified Munsell color charts when illuminated with reference light are plotted (Duv = −0.0500). Spectral distributions assumed to be emitted from packaged LEDs that contain four types of semiconductor light emitting elements and illuminate 15 types of modified Munsell color charts, and when illuminated with the LEDs and when illuminated with reference light It is a figure which shows the CIELAB color space which plotted together the a ^* value and b ^* value of the said 15 types of correction | amendment Munsell color charts (Duv = 0.0000). Spectral distributions assumed to be emitted from packaged LEDs that contain four types of semiconductor light emitting elements and illuminate 15 types of modified Munsell color charts, and when illuminated with the LEDs and when illuminated with reference light It is a figure which shows the CIELAB color space which plotted together the a ^* value and b ^* value of the said 15 types of correction Munsell color charts (Duv = 0.0100). Spectral distributions assumed to be emitted from packaged LEDs that contain four types of semiconductor light emitting elements and illuminate 15 types of modified Munsell color charts, and when illuminated with the LEDs and when illuminated with reference light It is a figure which shows the CIELAB color space which plotted both a ^* value and b ^* value of the said 15 types of correction | amendment Munsell color charts (Duv = 0.0200). Spectral distributions assumed to be emitted from packaged LEDs that contain four types of semiconductor light emitting elements and illuminate 15 types of modified Munsell color charts, and when illuminated with the LEDs and when illuminated with reference light It is a figure which shows the CIELAB color space which plotted together the a ^* value and b ^* value of the said 15 types of correction Munsell color charts (Duv = 0.0300). Spectral distributions assumed to be emitted from packaged LEDs that contain four types of semiconductor light emitting elements and illuminate 15 types of modified Munsell color charts, and when illuminated with the LEDs and when illuminated with reference light It is a figure which shows the CIELAB color space which plotted both a ^* value and b ^* value of the said 15 types of correction Munsell color charts (Duv = 0.0400). Spectral distributions assumed to be emitted from packaged LEDs that contain four types of semiconductor light emitting elements and illuminate 15 types of modified Munsell color charts, and when illuminated by the LEDs and when illuminated by reference light It is a figure which shows the CIELAB color space which plotted both a ^* value and b ^* value of the said 15 types of correction | amendment Munsell color charts (Duv = -0.0100). Spectral distributions assumed to be emitted from packaged LEDs that contain four types of semiconductor light emitting elements and illuminate 15 types of modified Munsell color charts, and when illuminated by the LEDs and when illuminated by reference light It is a figure which shows the CIELAB color space which plotted both a ^* value and b ^* value of the said 15 types of correction | amendment Munsell color charts (Duv = -0.0200). Spectral distributions assumed to be emitted from packaged LEDs that contain four types of semiconductor light emitting elements and illuminate 15 types of modified Munsell color charts, and when illuminated by the LEDs and when illuminated by reference light It is a figure which shows the CIELAB color space which plotted both a ^* value and b ^* value of the said 15 types of correction | amendment Munsell color charts (Duv = -0.0300). Spectral distributions assumed to be emitted from packaged LEDs that contain four types of semiconductor light emitting elements and illuminate 15 types of modified Munsell color charts, and when illuminated by the LEDs and when illuminated by reference light It is a figure which shows the CIELAB color space which plotted both a ^* value and b ^* value of the said 15 types of correction | amendment Munsell color charts (Duv = -0.0400). Spectral distributions assumed to be emitted from packaged LEDs that contain four types of semiconductor light emitting elements and illuminate 15 types of modified Munsell color charts, and when illuminated by the LEDs and when illuminated by reference light It is a figure which shows the CIELAB color space which plotted both a ^* value and b ^* value of the said 15 types of correction | amendment Munsell color charts (Duv = -0.0500). A spectral distribution assuming that a semiconductor light emitting element having a peak wavelength of 405 nm is embedded, emitted from a package LED including a blue phosphor, a green phosphor, and a red phosphor and illuminating 15 kinds of modified Munsell color charts, and the LED FIG. 6 is a diagram showing a CIELAB color space in which a ^* values and b ^* values of the 15 types of modified Munsell color charts when illuminated with reference light and when illuminated with reference light are plotted (Duv = 0.0). 0001). A spectral distribution assuming that a semiconductor light emitting element having a peak wavelength of 405 nm is embedded, emitted from a package LED including a blue phosphor, a green phosphor, and a red phosphor and illuminating 15 kinds of modified Munsell color charts, and the LED FIG. 6 is a diagram showing a CIELAB color space in which a ^* values and b ^* values of the 15 types of modified Munsell color charts when illuminated with reference light and when illuminated with reference light are plotted (Duv = 0.0). 0100). A spectral distribution assuming that a semiconductor light emitting element having a peak wavelength of 405 nm is embedded, emitted from a package LED including a blue phosphor, a green phosphor, and a red phosphor and illuminating 15 kinds of modified Munsell color charts, and the LED FIG. 6 is a diagram showing a CIELAB color space in which a ^* values and b ^* values of the 15 types of modified Munsell color charts when illuminated with reference light and when illuminated with reference light are plotted (Duv = 0.0). 0194). A spectral distribution assuming that a semiconductor light emitting element having a peak wavelength of 405 nm is embedded, emitted from a package LED including a blue phosphor, a green phosphor, and a red phosphor and illuminating 15 kinds of modified Munsell color charts, and the LED FIG. 6 is a diagram showing a CIELAB color space in which a ^* values and b ^* values of the 15 types of modified Munsell color charts when illuminated with reference light and when illuminated with reference light are plotted (Duv = 0.0). 0303). A spectral distribution assuming that a semiconductor light emitting element having a peak wavelength of 405 nm is embedded, emitted from a package LED including a blue phosphor, a green phosphor, and a red phosphor and illuminating 15 kinds of modified Munsell color charts, and the LED FIG. 6 is a diagram showing a CIELAB color space in which a ^* values and b ^* values of the 15 types of modified Munsell color charts when illuminated with reference light and when illuminated with reference light are plotted (Duv = 0.0). 0401). A spectral distribution assuming that a semiconductor light emitting element having a peak wavelength of 405 nm is embedded, emitted from a package LED including a blue phosphor, a green phosphor, and a red phosphor and illuminating 15 kinds of modified Munsell color charts, and the LED FIG. 6 is a diagram showing a CIELAB color space in which a ^* values and b ^* values of the 15 types of modified Munsell color charts when illuminated with reference light and when illuminated with reference light are plotted (Duv = 0.0). 0496). A spectral distribution assuming that a semiconductor light emitting element having a peak wavelength of 405 nm is embedded, emitted from a package LED including a blue phosphor, a green phosphor, and a red phosphor and illuminating 15 kinds of modified Munsell color charts, and the LED FIG. 6 is a diagram showing a CIELAB color space in which a ^* values and b ^* values of the 15 kinds of modified Munsell color charts when illuminated with reference light and when illuminated with reference light are plotted (Duv = −0). .0100). A spectral distribution assuming that a semiconductor light emitting element having a peak wavelength of 405 nm is embedded, emitted from a package LED including a blue phosphor, a green phosphor, and a red phosphor and illuminating 15 kinds of modified Munsell color charts, and the LED FIG. 6 is a diagram showing a CIELAB color space in which a ^* values and b ^* values of the 15 kinds of modified Munsell color charts when illuminated with reference light and when illuminated with reference light are plotted (Duv = −0). 0.0200). A spectral distribution assuming that a semiconductor light emitting element having a peak wavelength of 405 nm is embedded, emitted from a package LED including a blue phosphor, a green phosphor, and a red phosphor and illuminating 15 kinds of modified Munsell color charts, and the LED FIG. 6 is a diagram showing a CIELAB color space in which a ^* values and b ^* values of the 15 kinds of modified Munsell color charts when illuminated with reference light and when illuminated with reference light are plotted (Duv = −0). .0303). A spectral distribution assuming that a semiconductor light emitting element having a peak wavelength of 405 nm is embedded, emitted from a package LED including a blue phosphor, a green phosphor, and a red phosphor and illuminating 15 kinds of modified Munsell color charts, and the LED FIG. 6 is a diagram showing a CIELAB color space in which a ^* values and b ^* values of the 15 kinds of modified Munsell color charts when illuminated with reference light and when illuminated with reference light are plotted (Duv = −0). 0.0403). Built-in semiconductor light emitting device with a peak wavelength of 405 nm, emitted from a package LED including a blue phosphor and a red phosphor, a spectral distribution assumed to have illuminated 15 types of modified Munsell color charts, and illuminated with the LED And CIELAB color space in which a ^* values and b ^* values of the 15 types of modified Munsell color charts when illuminated with reference light are plotted (Duv = −0.0448). It is a figure which shows the integration range of parameter _Acg (when CCT is 5000K or more). It is a figure which shows the integration range of parameter _Acg (when CCT is less than 5000K). FIG. 3 is a diagram illustrating a normalized test light spectral distribution (solid line) of the test light 5 and a normalized reference light spectral distribution (dotted line) of the calculation reference light corresponding to the test light 5; The a ^* value and b ^* value of the 15 types of corrected Munsell color charts, assuming that the object is illuminated with the test light 5 (solid line) and that the object is illuminated with the reference light for calculation corresponding to the test light 5 respectively. FIG. 6 is a diagram illustrating a CIELAB color space in which both are plotted. FIG. 3 is a diagram illustrating a normalized test light spectral distribution (solid line) of the test light 15 and a normalized reference light spectral distribution (dotted line) of the calculation reference light corresponding to the test light 15. The a ^* value and b ^* value of the 15 types of modified Munsell color charts assuming that the object is illuminated with the test light 15 (solid line) and the case where the object is illuminated with the calculation reference light corresponding to the test light 15 respectively. FIG. 6 is a diagram illustrating a CIELAB color space in which both are plotted. FIG. 3 is a diagram illustrating a normalized test light spectral distribution (solid line) of the test light 19 and a normalized reference light spectral distribution (dotted line) of the calculation reference light corresponding to the test light 19; The a ^* value and b ^* value of the 15 types of corrected Munsell color charts, assuming that the object is illuminated with the test light 19 (solid line) and the case where the object is illuminated with the calculation reference light corresponding to the test light 19 respectively. FIG. 6 is a diagram illustrating a CIELAB color space in which both are plotted. FIG. 4 is a diagram showing a normalized test light spectral distribution (solid line) of the comparative test light 14 and a normalized reference light spectral distribution (dotted line) of the calculation reference light corresponding to the comparative test light 14. The a ^* value and b of the fifteen kinds of corrected Munsell color charts, assuming that the object is illuminated with the comparative test light 14 (solid line) and the case where the object is illuminated with the reference light for calculation corresponding to the comparative test light 14 respectively. ^* CIELAB color space with values plotted together. It is a schematic diagram which shows an example of the light-emitting device which concerns on this embodiment. It is a schematic diagram which shows an example of the light-emitting device which concerns on this embodiment. It is a figure of the spectral distribution in Reference Example 1 and Example 1. In the figure, the dotted line indicates the relative total radiant flux spectral distribution in Reference Example 1 that does not include the control element, and the solid line indicates the relative spectral distribution emitted on the axis in Example 1 that includes the control element. Assuming the case where the relative total radiant flux spectral distribution from the packaged LED (without the control element) in FIG. It is a CIELAB plot in which a ^* values and b ^* values of 15 color charts are plotted. (The dotted line in the figure is the result of the reference light, and the solid line in the figure is the result of the package LED). The relative spectral distribution radiated on the axis from the light emitting device (with a control element) according to the embodiment of the present invention of FIG. It is a CIELAB plot in which the a ^* value and the b ^* value of the 15 color chart are plotted together assuming the respective illumination cases. (The dotted line in the figure is the result of the reference light, and the solid line in the figure is the result of the light emitting device). It is a figure of the spectral distribution in Reference Example 2 and Example 2. In the figure, the dotted line indicates the relative total radiant flux spectral distribution in Reference Example 2 that does not include the control element, and the solid line indicates the relative spectral distribution emitted on the axis in Example 2 that includes the control element. It is assumed that the relative total radiant flux spectral distribution from the packaged LED (without control element) in FIG. 48 and the calculation reference light (black body radiation light) having the corresponding CCT are respectively illuminated. It is a CIELAB plot in which a ^* values and b ^* values of 15 color charts are plotted. (The dotted line in the figure is the result of the reference light, and the solid line in the figure is the result of the package LED). The relative spectral distribution emitted on the axis from the light emitting device (with control element) according to the embodiment of the present invention in FIG. 48 and the calculation reference light (black body radiation light) having the corresponding CCT, It is a CIELAB plot in which the a ^* value and b ^* value of the 15 color chart are plotted together assuming the case where each is illuminated. (The dotted line in the figure is the result of the reference light, and the solid line in the figure is the result of the light emitting device). It is a figure of the spectral distribution in Reference Example 3 and Example 3. In the figure, the dotted line indicates the relative total radiant flux spectral distribution in Reference Example 3 that does not include the control element, and the solid line indicates the relative spectral distribution emitted on the axis in Example 3 that includes the control element. It is assumed that the relative total radiant flux spectral distribution from the packaged LED (without the control element) in FIG. It is a CIELAB plot in which a ^* values and b ^* values of 15 color charts are plotted. (The dotted line in the figure is the result of the reference light, and the solid line in the figure is the result of the package LED). 51. The relative spectral distribution emitted on the axis from the light emitting device (with control elements) according to the embodiment of the present invention in FIG. 51 and the calculation reference light (black body radiation light) having the corresponding CCT. It is a CIELAB plot in which the a ^* value and b ^* value of the 15 color chart are plotted together assuming the case where each is illuminated. (The dotted line in the figure is the result of the reference light, and the solid line in the figure is the result of the light emitting device). It is a figure of the spectral distribution in Reference Example 4 and Example 4. In the figure, the dotted line indicates the relative total radiant flux spectral distribution in Reference Example 4 that does not include the control element, and the solid line indicates the relative spectral distribution emitted on the axis in Example 4 that includes the control element. It is assumed that the relative total radiant flux spectral distribution from the package LED (without control element) in FIG. 54 and the calculation reference light (black body radiation light) having the corresponding CCT are respectively illuminated. It is a CIELAB plot in which a ^* values and b ^* values of 15 color charts are plotted. (The dotted line in the figure is the result of the reference light, and the solid line in the figure is the result of the package LED). 54, a relative spectral distribution radiated on the axis from the light emitting device (with a control element) according to the embodiment of the present invention in FIG. 54, and a calculation reference light (black body radiation light) having a corresponding CCT, It is a CIELAB plot in which the a ^* value and b ^* value of the 15 color chart are plotted together assuming the case where each is illuminated. (The dotted line in the figure is the result of the reference light, and the solid line in the figure is the result of the light emitting device). It is a figure of the spectral distribution in the reference comparative example 1 and the comparative example 1. FIG. In the figure, the dotted line indicates the relative total radiant flux spectral distribution of the incandescent lamp that is the reference comparative example 1 that does not include the control element, and the solid line is radiated on the axis in the neodymium lamp that is the comparative example 1 including the control element. Relative spectral distribution is shown. It is assumed that the relative total radiant flux spectral distribution from the incandescent bulb (without control element) in FIG. It is a CIELAB plot in which a ^* values and b ^* values of 15 color charts are plotted. (The dotted line in the figure is the result of the reference light, and the solid line in the figure is the result of the incandescent lamp). In the figure, the dotted line and the solid line overlap. It is assumed that the relative spectral distribution radiated on the axis from the neodymium bulb (with control elements) in FIG. 57 and the reference light for calculation (light of black body radiation) having the corresponding CCT are illuminated. FIG. 6 is a CIELAB plot in which the a ^* value and b ^* value of the 15 color chart are plotted together. (The dotted line in the figure is the result of the reference light, and the solid line in the figure is the result of the neodymium bulb).

Hereinafter, the present invention will be described in detail. However, the present invention is not limited to the following embodiments, and various modifications can be made without departing from the scope of the invention.
The light emitting device of the present invention includes a light emitting element and a control element.
The light-emitting element of the present invention is particularly limited as long as it is inherent in the light-emitting device, converts various input energy into electromagnetic radiation energy, and includes visible light of 380 nm to 780 nm in the electromagnetic radiation energy. Not. For example, a hot filament capable of converting electric energy, a fluorescent tube, a high-pressure sodium lamp, a laser, a semiconductor light emitting element (or LED), a second harmonic generation (SHG) source, and the like can be exemplified. Moreover, the fluorescent substance etc. which can convert light energy can also be illustrated.

  The control element of the present invention is a passive element that does not have an amplification function by itself, and is suitable for light emitted from a light emitting element or a light emitting device having a relatively low processing degree in a main direction. There is no particular limitation as long as intensity modulation for each wavelength can be applied within a range and a light-emitting device with a high degree of processing can be configured. For example, examples of the control element of the present invention include passive devices such as a reflection mirror, an optical filter, and various optical lenses. Further, the control element of the present invention may be a light-absorbing material that is dispersed in the sealing material of the package LED and gives intensity modulation for each wavelength within an appropriate range. However, the control element does not include a light-emitting element, a reflection mirror, an optical filter, a light-absorbing material, or the like that gives only intensity modulation with a small wavelength dependency to light emitted from a light-emitting device having a relatively low degree of processing.

  An outline of the light emitting device of the present invention will be further described with reference to FIG. In the example of FIG. 43, the LED chip 2 that is a semiconductor light emitting element and the phosphor 4 are incorporated as light emitting elements, and the package LED 10 that is a light emitting device with a low degree of processing together with the sealing material 6 and the package material 3 that are other constituent materials. Is configured. At this time, the optical filter 5 that gives intensity modulation for each wavelength in an appropriate range as a control device is installed in the light emission direction of the package LED 10 to constitute the LED bulb 20 that is a light-emitting device having a high degree of processing as a whole. The LED bulb 20 may be a light emitting device of the present invention.

  Furthermore, the outline of the light emitting device of the present invention will be further described with reference to FIG. A blue LED chip 2a, a green LED 2b chip, and a red LED chip 2c, which are semiconductor light emitting elements, are incorporated as light emitting elements, and a package LED 10 which is a light emitting device with a low degree of processing together with a sealing material 6 and a package material 3 which are other constituent materials. Is configured. At this time, the optical filter 5 that functions as a control device is installed in the radiation direction of the package LED 10 to constitute the LED bulb 20 that is a light emitting device having a high degree of processing as a whole. The LED bulb 20 may be the light emitting device of the present invention. Further, n LED light bulbs 20 are arranged, and m incandescent bulbs 11 are arranged as a light emitting device having a moderate degree of processing and a heat filament 2d as a light emitting element, and the illumination system 30 is configured as a light emitting device having a high degree of processing. To do. The illumination system can be the light emitting device of the present invention.

The total radiant flux emitted from the light-emitting elements described in this specification is the sum of all radiant fluxes emitted from all the light-emitting elements, and this spectral distribution is described as Φ _elm here. The Φ _elm is a function of the wavelength λ. The actual measurement of Φ _elm (λ) can be performed, for example, by performing radiation measurement using an integrating sphere in a form in which the control element described in this specification is excluded from the light emitting device. As shown in FIG. 43, in a light-emitting device having an LED filter and phosphor as a light-emitting element and having an optical filter that gives intensity modulation for each wavelength in an appropriate range as a control element, all of the forms excluding the optical filter are included. If the radiant flux spectral distribution is measured, Φ _elm (λ) is obtained. That is, Φ _elm (λ) can be obtained by measuring the total radiant flux spectral distribution of the package LED, which is a light-emitting device with a low degree of processing.
In addition, as shown in FIG. 44, if there is a “light emitting device with a high degree of processing or a light emitting device with a high degree of processing” that is partially present in the “light emitting device with a higher degree of processing”, the control element does not act. The sum of the total radiation of each of the n package LEDs and the m incandescent bulbs can be regarded as Φ _elm (λ).
Further, in Φ _elm (λ), when the maximum total radiant flux spectral intensity within the defined wavelength range is Φ _elmmax , and the wavelength to give this is λ _elmmax (nm), in this specification, the defined wavelength The relative spectral distribution of the light emitting element divided by the maximum total radiant flux spectral intensity within the range, that is, Φ _elm (λ) / Φ _elmmax is described as Φ _elmrel (λ). Here, as a matter of course, Φ _elmmax can have different values if the defined wavelength range is different.

On the other hand, in the first and second embodiments of the present invention, the total radiant flux spectral distribution Φ _elm (λ) of the light emitting element inherent in the light emitting device is affected by the control element inherent in the light emitting device, Thereafter, the invention is specified by the light emitted in the “main radiation direction”. Therefore, a light emitting device that can emit light including light in the “main radiation direction” that satisfies the requirements of the present invention under the action of the control element belongs to the scope of the present invention. In the illumination method according to the third embodiment of the present invention, when the light emitted from the light emitting device illuminates the object, the invention is specified by the light at the position where the object is illuminated. It is. Therefore, an illumination method using a light emitting device that can emit light at a “position where an object is illuminated” that satisfies the requirements of the present invention belongs to the scope of the present invention.

Here, the “main radiant direction” in the first and second embodiments of the present invention has a suitable range in accordance with the use state of the light emitting device and a suitable orientation. Indicates the direction in which light is emitted.
For example, it may be a direction in which the luminous intensity or luminance of the light emitting device is maximized or maximized.
Further, the light emitting device may have a finite range including a direction in which the luminous intensity or luminance of the light emitting device is maximized or maximized.
In addition, the radiant intensity or radiance of the light emitting device may be in the maximum or maximum direction.
Further, it may be a direction having a finite range including a direction in which the radiant intensity or radiance of the light emitting device is maximized or maximized.
Specific examples are given below.
When the light emitting device is a single light emitting diode (LED), a single package LED, a single LED module, a single LED bulb, a single composite lamp of a fluorescent lamp and a semiconductor light emitting element, a single composite lamp of an incandescent bulb and a semiconductor light emitting element, etc. The main radiation direction may be the vertical direction of each light emitting device and a finite solid angle including the vertical direction, for example, π (sr) at the maximum and π / 100 (sr) at the minimum.
The light emitting device is an LED lighting device in which a lens, a reflection mechanism or the like is added to the package LED or the like, a lighting device including a fluorescent lamp and a semiconductor light emitting element, and so-called direct type lighting use, semi-direct type lighting use, general diffusion In the case of light distribution characteristics applicable to lighting applications, direct / indirect lighting applications, semi-indirect lighting applications, and indirect lighting applications, the main radiation direction is finite including the vertical direction and vertical direction of each light emitting device For example, π (sr) at the maximum and π / 100 (sr) at the minimum. In addition, the luminous intensity or luminance of the light emitting device may be in a direction that is maximized or maximized. Further, it may be within a finite solid angle including the direction in which the luminous intensity or luminance of the light emitting device is maximized or maximized, for example, π (sr) at the maximum and π / 100 (sr) at the minimum. In addition, the radiant intensity or radiance of the light emitting device may be in a direction that maximizes or maximizes. Further, it may be within a finite solid angle including a direction in which the radiant intensity or radiance of the light emitting device is maximized or maximized, for example, π (sr) at the maximum and π / 100 (sr) at the minimum.
When the light-emitting device is a lighting system including a plurality of lighting fixtures including the LED lighting fixture and the fluorescent lamp, the main radiation direction is a vertical direction of the planar center of each light-emitting device and a finite number including the vertical direction. It can be within a solid angle, for example, π (sr) at the maximum and π / 100 (sr) at the minimum. In addition, the luminous intensity or luminance of the light emitting device may be in a direction that is maximized or maximized. Further, it may be within a finite solid angle including the direction in which the luminous intensity or luminance of the light emitting device is maximized or maximized, for example, π (sr) at the maximum and π / 100 (sr) at the minimum. In addition, the radiant intensity or radiance of the light emitting device may be in a direction that maximizes or maximizes. Further, it may be within a finite solid angle including a direction in which the radiant intensity or radiance of the light emitting device is maximized or maximized, for example, π (sr) at the maximum and π / 100 (sr) at the minimum.
In order to measure the spectral distribution of the light emitted from the light emitting device in the main radiation direction, it is preferable to measure at a distance at which the illuminance at the measurement point becomes practical illuminance (150 lx to 5000 lx as described later).

Therefore, when the spectral distribution of light emitted from the light emitting device including the control element in the main radiation direction is φ _SSL (λ), the relative spectral distribution φ _SSLrel (λ of the light emitting device divided by φ _SSL (λ _elmmax ). ) (That is, φ _SSL (λ) / φ _SSL (λ _elmmax )) has the following meaning. Since lambda _Elmmax is a wavelength giving a maximum total radiant flux spectral intensity [Phi _Elmmax emitting element within a wavelength range defined as the relative spectral intensity phi _SSL of the light-emitting device in the _λ elmmax (λ elmmax), primary radiation from the light-emitting device That is, the spectral distribution φ _SSL (λ) of the light emitted in the direction is divided.

As a result, φ _SSLrel (λ) / Φ _elmrel (λ) has the following meaning. When it is 1.0 at an arbitrary λ within the defined wavelength range, the spectral distribution is not subjected to a relative change by the control element included in the light emitting device, and the total radiant flux spectrum emitted from the light emitting element is not affected. The shape of the distribution means that the light is emitted in the main radiation direction of the light emitting device while being preserved. For example, φ _SSLrel (λ) / Φ _elmrel (λ) before and after passing through an ND filter having a constant transmission characteristic in the visible light region is ideally 1.0.

Further, when φ _SSLrel (λ) / Φ _elmrel (λ) is in the vicinity of 1.0 at an arbitrary λ within the defined wavelength range, the action of the control element inherent in the light emitting device is weak, The shape of the total radiant flux spectral distribution emitted from the light emitting element means that it is emitted in the main radiation direction of the light emitting device with little change.

On the other hand, if φ _SSLrel (λ) / Φ _elmrel (λ) is significantly different from 1.0 at least at a certain specific λ within the defined wavelength range, or λ within the specific range, The action of the control element inherent in the light emitting element is strong, which means that the shape of the total radiant flux spectral distribution emitted from the light emitting element is emitted in the main radiation direction of the light emitting device in response to a large change.

In this specification, the reference light defined by the CIE used for calculation when predicting the appearance of mathematical colors may be described as reference light, calculation reference light, calculation reference light, or the like. is there. On the other hand, the experimental reference light used in the actual visual comparison, that is, the incandescent bulb light including the tungsten filament, may be described as the reference light, the experimental reference light, and the experimental reference light. Further, light having a high _Ra and high _Ri, which is expected to have a color appearance close to the reference light, for example, an LED light source, which is used as a substitute light for the experimental reference light in the comparative visual experiment, Sometimes referred to as reference light, experimental pseudo-reference light, and experimental pseudo-reference light. In addition, light that is mathematically and experimentally studied may be described as test light with respect to reference light.

  The light emitting device according to the first embodiment of the present invention includes a light emitting element. Moreover, the light-emitting device used for the illumination method according to the third embodiment of the present invention includes a light-emitting element. The light emitting element is not particularly limited as long as it can emit light corresponding to a range of 380 nm to 780 nm by any method. For example, the light emitted from a heat filament or the like, from a fluorescent tube, a high pressure sodium lamp, or the like. Examples thereof include discharge radiation light, stimulated emission light from a laser, spontaneous emission light from a semiconductor light emitting element, spontaneous emission light from a phosphor, and the like. The light emitting device according to this embodiment also includes a control element, but other configurations are not particularly limited. However, the light emitting element included in the light emitting device according to the first embodiment of the present invention or the light emitting element included in the light emitting device used in the illumination method according to the third embodiment of the present invention includes a semiconductor light emitting element. It is preferable. Therefore, for example, when a semiconductor light emitting device is included as a light emitting element, even if the light emitting element is a single semiconductor light emitting element provided with a lead wire or the like as an energization mechanism, it is further provided with a heat dissipation mechanism or the like to be integrated with a phosphor or the like. A packaged LED or the like may be used. Further, an LED module in which a more robust heat dissipation mechanism is provided to one or more packaged LEDs and a plurality of packaged LEDs are mounted may be used. Furthermore, the LED lighting fixture which provided the lens, the reflection mechanism, etc. to package LED etc. may be sufficient. Furthermore, the lighting system which supported many LED lighting fixtures etc. and was able to illuminate a target object may be sufficient. Further, for example, in the case where a discharge tube is included as a light emitting element, the light emitting device according to this embodiment is provided with a mechanism capable of applying a high voltage to a single discharge tube, but a phosphor is disposed in or around the discharge tube. You may have done. Further, it may be a lighting fixture in which a plurality of fluorescent tubes containing one or more fluorescent materials are arranged. Furthermore, the lighting fixture which provided the reflection mechanism etc. may be sufficient. Furthermore, you may provide a control circuit etc. by making this into an illumination system. The light emitting device according to this embodiment includes all of them.

Hereinafter, the present invention will be described in detail.
The present inventor has a natural, lively, highly visible, comfortable, color appearance, and object appearance as seen in an outdoor high illumination environment even in a general indoor illumination environment. We have found radiometric properties and photometric properties common to spectra or spectral distributions that can realize the above. Furthermore, how the color chart's color appearance having specific spectral reflection characteristics when illumination with light having the spectrum or spectral distribution is assumed is compared to when illumination with calculation reference light is assumed. From the viewpoint of colorimetry, it was found whether the object can be realized when it changes (or does not change).
In addition, for example, even if lighting objects are concerned about side effects due to light irradiation, such as fine arts, fresh foods, etc., natural, lively, highly visible, comfortable, The spectral distribution of a light-emitting device that can achieve both color appearance, object appearance, and suppression of the secondary effects has been studied, and the present invention as a whole has reached the present invention.
The outline until the specific invention was achieved was as follows.

[Outline of Invention]
As a first step, the function of the control element is not taken into account, and the degree of freedom of setting the spectral distribution is high. Assuming a packaged LED light source that has only a light emitting element as a light emitting element, a mathematical basic study was performed.
At this time, a guideline is provided for mathematical changes in the color appearance of the color chart having a specific spectral reflection characteristic between the case of assuming illumination with the reference light for calculation and the case of illumination using the test light to be studied. However, detailed examination was performed on test light in which hue, saturation (saturation), and the like change. Especially focusing on the light that changes the saturation of the color appearance of the illuminated object, considering the hunt effect in a normal indoor environment where the illuminance decreases from 1/10 to 1/1000 compared to the outdoors Mathematically examined.

As a second step, a packaged LED light source based on the test light mathematically examined, and a lighting fixture incorporating the packaged LED light source, were produced. The luminaire did not include a control element function. In addition, an incandescent bulb having a tungsten filament was prepared as an experimental reference light for a comparative visual experiment performed in the third step. The calculation reference of the light source may be a light (experimental pseudo reference light) becomes color appearance close to light the high R _a and high R _i, also the prototype luminaire inherent this. Furthermore, for visual experiments using these, the color appearance when the object is illuminated with the experimental reference light or the experimental pseudo reference light, and the light (test light) of the luminaire with the package LED light source included In order to have the subject evaluate the appearance of the color when the object is illuminated, an illumination experiment system capable of irradiating different illumination lights to a large number of observation objects was created.

  As a third step, a comparative visual experiment was performed using a lighting apparatus and a lighting system that do not have the function of the control element. As for the color of the observation target, consideration was given to preparing a chromatic color target covering all hues such as purple, blue-violet, blue, blue-green, green, yellow-green, yellow, yellow-red, red, red-purple. Furthermore, achromatic objects such as white and black were also prepared. Many kinds of these were prepared such as still life, fresh flowers, food, clothing and printed matter. Here, the subject evaluated the color appearance when the object was illuminated with the experimental reference light or the experimental reference light and the color appearance when the object was illuminated with the test light. Comparison between the former and the latter was performed with similar CCT and similar illuminance. The evaluation is performed from the viewpoint of which light, which is natural, lively, highly visible, comfortable, color appearance, and object appearance, as seen outdoors, can be realized. received. At the same time, he asked why he was superior or inferior.

  As a fourth step, the radiometric characteristics and photometric characteristics of the experimental reference light / experimental pseudo reference light and the test light were extracted from the actual measurement values. Furthermore, regarding the colorimetric characteristics relating to the color appearance of the color chart having a specific spectral reflection characteristic, which is different from the above-mentioned observation object, when the calculation light is assumed to be calculated with the spectral distribution of the reference light for calculation, and the actual measurement Illumination that is judged to be truly comfortable by comparing the difference between the calculated experimental reference light / experimental pseudo-reference light / test light with the spectrally distributed light and the assumption of calculation in the visual test. The characteristics of the method or light emitting device were extracted.

Further, as a fifth step, a study was conducted to introduce a control element into a light emitting device that does not include the control element.
The contents of the third step and the fourth step are reference examples and reference comparative examples according to the first and second embodiments of the present invention, and the contents of the fifth step are the first and second steps of the present invention. It is also an Example and a comparative example according to the second embodiment. The contents of the second step, the third step, the fourth step, and the fifth step are reference examples and reference comparative examples according to the third embodiment of the present invention, and the content of the fifth step is the present invention. This is also an example and a comparative example according to the third embodiment.

[Color chart selection and color appearance quantification method]
In the first step, the light mainly emitted from the light emitting device studied in the illumination method of the present invention has the spectral distribution at the position where the object is illuminated, or the light in the main radiation direction emitted from the light emitting device of the present invention. In consideration of the hunt effect, the spectral distribution is assumed to change from the case of illumination with the reference light. Here, the following selections were made to quantify the color appearance and its changes.

In order to quantitatively evaluate the color appearance from the above spectral distribution, a color chart with a clear mathematical spectral reflection characteristic is defined, and the illumination with the calculation reference light is assumed, and the illumination with the test light is performed. We compared the assumed cases and thought that it would be better to use the difference in color appearance of the color chart as an index.
In general, the test colors used in CRI can be an option, but the R ₁ to R ₈ color charts used when deriving the average color rendering index and the like are medium saturation color charts and have high saturation. I thought it was not suitable for discussing the saturation of various colors. R ₉ to R ₁₂ are highly saturated color charts, but the number of samples is insufficient for a detailed discussion of the entire hue angle range.

Therefore, in the Munsell hue circle in the modified Munsell color system, 15 types of color charts are selected for each hue from the color charts located at the outermost periphery with the highest saturation. These are based on the US NIST (National Institute of Standards and
This is the same as the color chart used in CQS (Color Quality Scale) (versions 7.4 and 7.5), which is one of the new color rendering evaluation indices proposed by Technology). The fifteen types of color charts used in the present invention are listed below. At the beginning, the number given to the color chart for convenience is shown. In the present specification, these numbers may be represented as n. For example, n = 3 means “5PB 4/12”. n is a natural number from 1 to 15.
# 01 7.5 P 4/10
# 02 10 PB 4/10
# 03 5 PB 4/12
# 04 7.5 B 5/10
# 05 10 BG 6/8
# 06 2.5 BG 6/10
# 07 2.5 G 6/12
# 08 7.5 GY 7/10
# 09 2.5 GY 8/10
# 10 5 Y 8.5 / 12
# 11 10 YR 7/12
# 12 5 YR 7/12
# 13 10 R 6/12
# 14 5 R 4/14
# 15 7.5 RP 4/12

  In the present invention, from the viewpoint of derivation of various indices, the appearance of the colors of these 15 kinds of color charts is assumed between the case where illumination with calculation reference light is assumed and the case where illumination with test light is assumed. , How it changes (or does not change), even in a general indoor illuminance environment, as seen in an outdoor high illuminance environment. We tried to quantify whether it was high, comfortable, color appearance, or object appearance, and extracted it as the color rendering properties that the light-emitting device should have.

In addition, in order to quantitatively evaluate the appearance of a color mathematically derived from the spectral distribution, selection of a color space and selection of a color adaptation formula are also important. In the present invention, CIE 1976 L ^* a ^* b ^* (CIELAB), which is a uniform color space currently recommended by the CIE, was used. Furthermore, CCMCAT2000 (Color Measurement Committee's Chroma Adaptation Transform) is used for chromatic adaptation calculation.
of 2000).

[Chromaticity point derived from the spectral distribution of the light in the main radiation direction emitted from the light emitting device not including the control element or from the spectral distribution at the position where the object is illuminated]
In the first step, the selection of the chromaticity point of the light source is also important for making various prototypes of packaged LED light sources. The chromaticity derived from the light source, the spectral distribution at the position where the object is illuminated with the light from the light source, or the spectral distribution of the light in the main radiation direction emitted from the light emitting device is, for example, CIE 1931 (x, y) Although it can be defined by a chromaticity diagram, it is preferable to discuss with a CIE 1976 (u ′, v ′) chromaticity diagram which is a more uniform chromaticity diagram. In addition, when describing the position on the chromaticity diagram in CCT and D _uv , the (u ′, (2/3) v ′) chromaticity diagram (synonymous with the CIE 1960 (u, v) chromaticity diagram) is used. Used. Note that D _uv described in this specification is an amount defined by ANSI C78.377, and is (u ′, (2/3) v ′) with respect to the black body radiation locus in the chromaticity diagram. The closest distance is shown as its absolute value. The positive sign indicates that the chromaticity point of the light emitting device is located above the black body radiation locus (v ′ is larger), and the negative sign indicates that the chromaticity point of the light emitting device is below the black body radiation locus (v ′ is small). Means to be located on the side).

[Calculation study on saturation and D _uv value]
Even at the same chromaticity point, the color appearance of the object can be changed. For example, the three types of spectral distributions (test light) shown in FIGS. 1, 2, and 3 include a semiconductor light emitting device having a peak wavelength of 425 to 475 nm, which is excited by a green phosphor and a red phosphor. This is an example in which the appearance of the color of the illuminated object is different at the same chromaticity (CCT is 5500K, D _uv is 0.0000), assuming a package LED as a light source. The green phosphor and the red phosphor constituting the respective spectral distributions are assumed to be the same material, but the peak wavelength of the blue semiconductor light emitting device is 459 nm in FIG. 1, 475 nm in FIG. In FIG. 3, it was 425 nm. Assuming illumination in each spectral distribution and illumination with a calculation reference light corresponding to the spectral distribution, the expected color appearance of the 15 color chart is shown in the CIELAB color space of FIGS. It becomes like. Here, the points connected by dotted lines in the figure are cases where illumination with calculation reference light is assumed, and the solid lines are cases where illumination with respective test lights is assumed. In addition, although the vertical direction on the paper is lightness, only the a ^* and b ^* axes are plotted here for convenience.

The following was found with respect to the spectral distribution shown in FIG. From the calculations assuming illumination with the reference light for calculation and the calculations assuming illumination with the test light in the figure, the appearance of the colors of the 15 color charts was expected to be close. Further, Ra calculated from the spectral distribution was as high as 95. In the case of assuming that the test light shown in FIG. 2 is illuminated, red and blue appear to be vivid, but purple and green are dull compared to the case of assuming that the sample is illuminated with the reference light for calculation. It was. Ra calculated from the spectral distribution was as low as 76. On the contrary, when it is assumed that the test light shown in FIG. 3 is illuminated, purple and green appear more vivid than red light when compared with the assumption that the reference light for calculation is illuminated. Was expected. Ra calculated from the spectral distribution was as low as 76.
Thus, it can be understood that the appearance of the color can be changed at the same chromaticity point.

However, according to the detailed examination by the present inventor, the light near the locus of blackbody radiation, that is, the light near D _uv is 0, the spectral distribution is changed, and the color of the 15 color chart having high saturation is seen. It turns out that the degree of freedom is low to change. Specifically, it was as follows.

For example, as shown in FIG. 2 and FIG. 3, it was predicted that the red / blue saturation change and the purple / green saturation change have opposite trends. That is, when the saturation of one hue is improved, the saturation of another hue is expected to decrease. From another study, it has also been difficult to change the saturation of the majority of hues at once using a simple and feasible method. Therefore, when illuminated with light in the vicinity of a blackbody radiation locus or light near D _uv = 0, the saturation of the majority of hues of the high-saturation 15 color chart is changed at once, or many hues are used. However, it was difficult to improve and reduce the saturation level relatively evenly.

Therefore, the present inventor mathematically compares the appearance of the color of the 15 color chart when different D _uv values are given to a plurality of spectral distributions with a case where illumination with calculation reference light is assumed. It was examined. Generally, when D _uv is positively biased, white appears to be greenish, when D _uv is negative, white appears to be reddish, and when D _uv is away from 0, the color appearance is unnatural as a whole. It is supposed to be visible. In particular, white coloration is believed to induce such perception. However, the present inventor has conducted the following studies in order to improve the controllability of the saturation.

The eight spectral distributions shown in FIGS. 4 to 11 include a blue semiconductor light emitting element having a peak wavelength of 459 nm, which is assumed to be a package LED using an excitation light source of a green phosphor and a red phosphor. This is a calculation result when D _uv is changed from −0.0500 to +0.0150 at (2700 K). The appearance of the colors of the 15 color charts expected when illumination with each spectral distribution (test light) is assumed and when illumination with calculation reference light for each test light is assumed is shown in FIG. It was as shown in CIELAB color space in FIG. Here, the points connected by dotted lines in the figure are the results of the calculation reference light, and the solid lines are the results of the respective test lights. In addition, although the vertical direction on the paper is lightness, only the a ^* and b ^* axes are plotted here for convenience.

In the test light with D _uv = 0.0000 shown in FIG. 4, when the illumination with the calculation reference light is assumed and when the illumination with the test light in the figure is assumed, the 15 kinds of color charts The color appearance was expected to be close. Ra calculated from the spectral distribution was as high as 95.

The test light in FIGS. 5 and 6 is an example in which D _uv is shifted in the positive direction from +0.0100 to +0.0150. As can be seen here, shifting D _uv in the positive direction changes the saturation of the 15 color charts in a wider hue range compared to the test light with D _uv = 0.0000. It was expected to be able to. It was also found that the saturation of the 15 types of color charts can be changed relatively evenly as compared with the test light with D _uv = 0.0000. In addition, in the case of the reference light for calculation and the case of the test light in the figure, the appearance of the colors of the 15 kinds of color charts is excluding the blue-blue region when D _uv is shifted in the positive direction. It was expected that almost all colors would appear dull. Furthermore, it was also predicted that the saturation level decreased as D _uv became positive. Ra calculated from the spectral distributions of FIGS. 5 and 6 was 94 and 89, respectively.

On the other hand, the test light in FIGS. 7 to 11 is an example in which D _uv is shifted in the negative direction from −0.0100 to −0.0500. As can be seen, shifting D _uv in the negative direction changes the saturation of the 15 color charts in a wider hue range compared to the test light with D _uv = 0.0000. It turns out that it can be made. It was also found that the saturation of the 15 types of color charts can be changed relatively evenly as compared with the test light with D _uv = 0.0000. Incidentally, in the case of assuming the lighting calculation reference light, in assuming a illumination with test light in the figure, see the color of the 15 kinds of color chips shifted the D _uv in the negative direction It was expected that almost all colors would look vivid except for the blue-to-blue-green region and the purple region. Further, it was predicted that the saturation level increased as D _uv was made negative. Ra calculated from the spectral distributions of FIGS. 7 to 11 are 92, 88, 83, 77, and 71, respectively, and according to an understanding that is currently widespread, the more negative the value of D _uv is, The color appearance was expected to be far from the case of illumination with reference light.

In addition, when the present inventors give various D _uv values to test light having different light-emitting elements (light-emitting materials) forming a spectrum, the most vivid 15-color chart at the outermost periphery of the modified Munsell color system What kind of color is expected to appear is examined mathematically while comparing with the reference light for calculation.

The 10 types of spectral distributions shown in FIG. 12 to FIG. 21 are obtained by changing D _uv from −0.0500 to +0.0400 in the same CCT (4000K) assuming a package LED containing four types of semiconductor light emitting elements. It is a result. The peak wavelengths of the four types of semiconductor light emitting devices were 459 nm, 528 nm, 591 nm, and 662 nm. Figure 10 shows the expected color appearance of the 15 color charts when assuming illumination with 10 types of test light and assuming illumination with reference light for calculation corresponding to each test light. 12 to CIELAB color space of FIG. Here, the points connected by the dotted lines in the figure are the results of the calculation reference light, and the solid lines are the results of the respective test lights. In addition, although the vertical direction on the paper is lightness, only the a ^* and b ^* axes are plotted here for convenience.

In the test light with D _uv = 0.0000 shown in FIG. 12, the 15 types of color charts are assumed when illumination with calculation reference light is assumed and when illumination with test light in the figure is assumed. The color appearance of was expected to be close. Ra calculated from the spectral distribution was as high as 98.

The test light in FIGS. 13 to 16 is an example in which D _uv is shifted in the positive direction from +0.0100 to +0.0400. As can be seen here, shifting D _uv in the positive direction changes the saturation of the 15 color charts in a wider hue range compared to the test light with D _uv = 0.0000. It turns out that it can be made. It was also found that the saturation of the 15 types of color charts can be changed relatively evenly as compared with the test light with D _uv = 0.0000. Incidentally, in the case of assuming the lighting calculation reference light, in the case of assuming the illumination with test light in the figure, see the color of the 15 kinds of color chips shifted the D _uv in the forward direction In this case, it was expected that almost all colors would appear dull, except for the blue to blue-green region and the red region. Furthermore, it was also predicted that the saturation level decreased as D _uv became positive. The Ra calculated from the spectral distributions of FIGS. 13 to 16 is 95, 91, 86, and 77, respectively, and according to the current general understanding, the more positive the value of D _uv , the more visible the color. Was expected to get worse and far from being illuminated with reference light.

On the other hand, the test light in FIGS. 17 to 21 is an example in which D _uv is shifted in the negative direction from −0.0100 to −0.0500. As can be seen, shifting D _uv in the negative direction changes the saturation of the 15 color charts in a wider hue range compared to the test light with D _uv = 0.0000. It turns out that it can be made. It was also found that the saturation of the 15 types of color charts can be changed relatively evenly as compared with the test light with D _uv = 0.0000. Incidentally, in the case of assuming the lighting calculation reference light, in assuming a illumination with test light in the figure, see the color of the 15 kinds of color chips shifted the D _uv in the negative direction In the case, it was expected that almost all colors would look vivid except for the blue-to-blue-green region and the red region. Further, it was predicted that the saturation level increased as D _uv was made negative. Ra calculated from the spectral distributions of FIGS. 17 to 21 are 95, 91, 86, 81, and 75, respectively, and according to the understanding that is currently widespread, the more negative the value of D _uv is, The color appearance was expected to be far from the case of illumination with reference light.

In addition, the present inventor has shown that the most vivid 15 colors in the outermost circumference of the modified Munsell color system when the light emitting elements (luminescent materials) forming the spectrum give different D _uv values to different test lights. We examined mathematically what kind of color the votes are expected to look, comparing with the reference light for calculation.

The 11 types of spectral distributions shown in FIG. 22 to FIG. 32 are adjacent to each other, assuming a package LED in which a purple semiconductor light emitting element is inherently used as an excitation light source of a blue phosphor, a green phosphor, and a red phosphor. This is a calculation result obtained by changing D _uv from −0.0448 to +0.0496 in CCT (about 5500 K). The peak wavelength of the incorporated semiconductor light emitting device was 405 nm. Note that the result of FIG. 32 is a result realized without including a green phosphor so that D _uv is extremely negative. The appearance of the color of the fifteen color charts predicted mathematically when assuming illumination with test light for each of the 11 types and assuming illumination with reference light for calculation with respect to the test light is shown in FIG. This is as shown in the CIELAB color space of FIG. Here, the points connected by dotted lines in the figure are the results of the calculation reference light, and the solid lines are the results of the respective test lights. In addition, although the vertical direction on the paper is lightness, only the a ^* and b ^* axes are plotted here for convenience.

In the test light with D _uv = 0.0001 shown in FIG. 22, the appearance of the colors of the 15 color charts is expected to be close in the case of the reference light for calculation and the case of the test light in the figure. It was. Ra calculated from the spectral distribution was as high as 96.

The test light in FIGS. 23 to 27 is an example in which D _uv is shifted in the positive direction from +0.0100 to +0.0496. As can be seen here, shifting D _uv in the positive direction changes the saturation of the 15 color charts in a wider hue range compared to the test light with D _uv = 0.0001. It turns out that it can be made. It was also found that the saturation of the 15 types of color charts can be changed relatively evenly as compared with the test light with D _uv = 0.0001. Incidentally, in the case of assuming the lighting calculation reference light, in assuming a illumination with test light in the figure, see the color of the 15 kinds of color chips shifted the D _uv in the forward direction In that case, it was expected that almost all colors would appear dull, except in the blue area. Furthermore, it was also predicted that the saturation level decreased as D _uv became positive. Ra calculated from the spectral distribution of FIG. 27 from FIG. 23, respectively 92,85,76,69,62, according to the understanding that now generally _spread, the more you positive value of _{D uv,} color The appearance of was far from being illuminated with the reference light, and was expected to deteriorate.

On the other hand, the test light in FIGS. 28 to 32 is an example in which D _uv is shifted in the negative direction from −0.0100 to −0.0448. As described above, D _uv = −0.0448 is realized as a system not including a green phosphor. As can be seen, shifting D _uv in the negative direction changes the saturation of the 15 color charts in a wider hue range compared to the test light with D _uv = 0.0001. It turns out that it can be made. It was also found that the saturation of the 15 types of color charts can be changed relatively evenly as compared with the test light with D _uv = 0.0001. Incidentally, in the case of assuming the lighting calculation reference light, in assuming a illumination with test light in the figure, see the color of the 15 kinds of color chips shifted the D _uv in the negative direction It was expected that almost all colors would look vivid except in the blue area. Further, it was predicted that the saturation level increased as D _uv was made negative. Ra calculated from the spectral distributions of FIGS. 28 to 32 are 89, 80, 71, 61, and 56, respectively. According to an understanding that is generally widespread at present, the more negative the value of D _uv is, The color appearance was expected to be far from the case of illumination with reference light.

[Summary of calculation study on saturation control and D _uv value]
From the calculation studies so far, the following was expected, "according to common sense now widely believed".
(1) With test light having a chromaticity point in the vicinity of D _uv = 0.0000, the degree of freedom to change the saturation of the 15 color chart is low. Specifically, it is difficult to change the saturation degree of the majority of hues of the 15 color charts having high saturation at once, or to improve or reduce the saturation degree relatively evenly in many hues.
(2) When the D _uv of the test light is positive, the saturation of the 15 color chart can be relatively easily reduced. Compared with the test light with D _uv = 0.0000, the saturation of the 15 types of color charts can be reduced in a wider hue range and relatively evenly. Furthermore, the more positive D _uv , the lower the saturation. In addition, since Ra is further reduced, in visual experiments and the like, the more the D _uv is made positive, the more the experimental illumination light or the like is illuminated with the experimental reference light and the test light. It was expected that the difference in the color appearance when illuminated with would be worse and worse. In particular, white was yellow (green), and the color appearance was expected to look unnatural.
(3) When D _uv is negative, the saturation of the 15-color chart can be increased relatively easily. Compared with the case of the test light with D _uv = 0.0000, the saturation of the 15 color charts can be improved in a wider hue range and relatively evenly. Further, as D _uv is made negative, the degree of saturation increases. In addition, since _Ra is further reduced, the more negative D _uv is, the case where the actual illumination object is illuminated with the experimental reference light or the experimental pseudo reference light, and the case where the test light is illuminated The difference in color appearance was expected to become worse and worse. In particular, the white color was red (pink), and the color appearance was expected to look unnatural.

  From the calculation so far, the above has been predicted "in light of common sense now widely believed".

[Introduction of quantitative indicators]
The following quantitative indicators were introduced in the present invention as preparation for discussing in detail the appearance of color, the characteristics of the spectral distribution itself, radiation efficiency, and the like, and as preparation for discussing in detail the appearance of color.
[Introduction of quantitative indicators related to color appearance]
First, the test light measured when the light emitting device emits the test light in the main radiation direction (according to the light emitting device of the present invention) or the position of the target when the target light is illuminated with the test light. The a ^* value and b ^* value of the 15 color _charts in the CIE 1976 L ^* a ^* b ^* color space of light (according to the illumination method of the present invention) are a ^* _nSSL and b ^* _nSSL (where n is 1). To 15), the hue angles of the 15 color _charts are set to θ _nSSL (degrees) (where n is a natural number from 1 to 15), and the calculation reference light selected according to the CCT of the test light. (less than 5000K is the blackbody radiation light, in the above 5000K the CIE daylight) of the 15 kinds of color chart in CIE 1976 L ^* a ^* b ^* color space when mathematically assuming an illumination by ^{a *} , ^{B *} values of each ^a _{* ^nref, b *} nref (where n is a natural number of 1 to 15), the 15 kinds of respective theta _nref the hue angle of the color chart (degrees) (where n is a natural number of 1 to 15) The absolute value of the hue angle difference Δh _n (degree) (where n is a natural number from 1 to 15) of each of the 15 types of modified Munsell color charts when illuminated with the two lights is | Δh _n | = | Θ _nSSL -θ _nref |
Defined.

  This is a visual test using test light and experimental reference light or experimental pseudo-reference light. As a means of realizing high, comfortable, color appearance and object appearance, the mathematically predicted hue angle difference related to the 15 kinds of modified Munsell color charts specially selected in the present invention is an important index. Because I thought.

（１）
さらに、当該１５種類の修正マンセル色票の飽和度差の最大値をΔＣ_ｍａｘ、飽和度差の最小値をΔＣ_ｍｉｎとした場合に、最大飽和度差と最小飽和度差の間の差（最大最小飽和度差間差）である
（ΔＣ_ｍａｘ−ΔＣ_ｍｉｎ）
も重要な指標と考えた。これは試験光と実験用基準光あるいは実験用擬似基準光を用いて視覚実験を行うに当たり、さまざまな物体、あるいは物体の色の見えを全体として評価し、自然で、生き生きとした、視認性の高い、快適な、色の見え、物体の見えを実現する手段として、本発明で特別に選択した当該１５種類の修正マンセル色票の飽和度差に関わる種々の特性は重要な指標になると考えたからである。 In addition, the saturation difference ΔC _n (where n is a natural number from 1 to 15) of the fifteen types of modified Munsell color charts assuming that the test light and the reference light for calculation are illuminated by two lights, respectively, ΔC _n = √ {(a ^* _nSSL ) ² + (b ^* _nSSL ) ² } −√ {(a ^* _nref ) ² + (b ^* _nref ) ² }
Defined. In addition, the following formula (1), which is an average value of the saturation difference of the 15 types of modified Munsell color charts, was also considered as an important index.

(1)
Further, when the maximum value of the saturation difference of the 15 types of modified Munsell color charts is ΔC _max and the minimum value of the saturation difference is ΔC _min , the difference between the maximum saturation difference and the minimum saturation difference (maximum Difference between minimum saturation differences) (ΔC _max −ΔC _min )
Also considered an important indicator. This is a visual test using test light and experimental reference light or experimental pseudo-reference light. As a means to realize high, comfortable, color appearance and object appearance, various characteristics related to the saturation difference of the 15 kinds of modified Munsell color charts specially selected in the present invention are considered to be important indicators. It is.

[Introduction of quantitative indicators for spectral distribution]
In the present invention, the following two quantitative indexes are introduced in order to discuss the radiometric characteristics and photometric characteristics of the spectral distribution. One is index A _cg and the other is radiation efficiency K (lm / W).

The index A _cg is the difference between the color appearance due to the experimental reference light or the experimental pseudo reference light and the color appearance due to the test light as a radiometric characteristic and a photometric characteristic of the spectral distribution or spectrum shape. I tried to describe it. As a result of various studies, the index A _cg is defined as follows in the present invention.

なお、ここで各積分の上下限波長は、それぞれ
Λ１＝３８０ｎｍ
Λ２＝４９５ｎｍ
Λ３＝５９０ｎｍ
とした。 Different when measuring light emitted in the main radiation direction from the light emitting device (according to the light emitting device of the present invention) or when measuring at the position of the illumination object (related to the illumination method of the present invention) Spectral distributions of the reference light for calculation and the test light that are color stimuli are respectively φ _ref (λ),
φ _SSL (λ), color matching functions x (λ), y (λ), z (λ), tristimulus values corresponding to the calculation reference light and test light (X _ref , Y _ref , Z _ref , respectively) ), (X _SSL , Y _SSL , Z _SSL ). Here, with respect to the reference light for calculation and the test light, the following holds, where k is a constant.
Y _ref = k∫φ _ref (λ) · y (λ) dλ
Y _SSL = k∫φ _SSL (λ) · y (λ) dλ
Here, the normalized spectral distribution obtained by normalizing the spectral distributions of the reference light for calculation and the test light with each Y is S _ref (λ) = φ _ref (λ) / Y _ref
S _SSL (λ) = φ _SSL (λ) / Y _SSL
And the difference between the normalized reference light spectral distribution and the normalized test light spectral distribution is expressed as ΔS (λ) = S _ref (λ) −S _SSL (λ)
It was. Furthermore, here, the index A _cg is defined as follows.

Here, the upper and lower limit wavelengths of each integral are Λ1 = 380 nm, respectively.
Λ2 = 495 nm
Λ3 = 590 nm
It was.

In addition, Λ4 was defined separately in the following two cases. First, in the normalized test light spectral segment S _SSL (λ), the wavelength giving the longest wavelength maximum value within 380 nm to 780 nm is λ _R (nm), and the spectral intensity is S _SSL (λ _R ). A wavelength that is on the longer wavelength side than λ _R and has an intensity of S _SSL (λ _R ) / 2 was defined as Λ4. If such a wavelength does not exist in the range up to 780 nm, Λ4 is set to 780 nm.

The indicator A _cg has a large visible range related to radiation that _causes color stimulation, a short wavelength region (or a blue region including purple), an intermediate wavelength region (a green region including yellow), and a long wavelength region (a red region including orange). This is an index that determines whether or not there is unevenness in the spectrum at an appropriate position in the standardized test light spectral distribution compared to the mathematical standardized standard light spectral distribution. is there. As illustrated in FIGS. 33 and 34, the long wavelength integration range varies depending on the position of the longest wavelength maximum value. Further, the selection of the reference light for calculation differs depending on the CCT of the test light. In the case of FIG. 33, since the CCT of the test light indicated by the solid line in the drawing is 5000K or more, CIE daylight (CIE daylight) is selected as the reference light as indicated by the dotted line in the drawing. In the case of FIG. 34, since the CCT of the test light indicated by a solid line in the drawing is less than 5000K, black body radiation light is selected as the reference light as indicated by the dotted line in the drawing. In the figure, the shaded portion schematically shows the integration range of the short wavelength region, the intermediate wavelength region, and the long wavelength region.

In the short wavelength region, the first term of the index A _cg (integral of ΔS (λ)) is a negative value when the spectral intensity of the normalized test light spectral distribution is stronger than the mathematical standardized reference light spectral distribution. It is easy to take. Conversely, in the intermediate wavelength region, when the spectral intensity of the standardized test light spectral distribution is weaker than the standardized reference light spectral distribution, the second term (integral of −ΔS (λ)) of the index A _cg is negative. Easy to take value. Further, in the long wavelength region, when the spectral intensity of the standardized test light spectral distribution is stronger than the standardized reference light spectral distribution, the third term (integral of ΔS (λ)) of the index A _cg has a negative value. It is an easy-to-take index.

Further, as described above, the calculation reference light is changed by the CCT of the test light. That is, as the reference light for calculation, black body radiation is used when the CCT of the test light is less than 5000K, and the defined CIE daylight (CIE daylight) is used when the CCT of the test light is 5000K or more. Used. In deriving the value of the index A _cg , φ _ref (λ) uses mathematically defined light of blackbody radiation or CIE daylight, while φ _SSL (λ) is the function used in the simulation, Or the value actually measured by experiment was used.

上記式において、
Ｋ_ｍ：最大視感度（ｌｍ／Ｗ）
Ｖ（λ）：分光視感効率
λ：波長（ｎｍ）
である。 Furthermore, when measuring light in the main radiation direction emitted from the light emitting device (according to the light emitting device of the present invention), or when measuring at the position of the illumination object (according to the illumination method of the present invention), In evaluating the test light spectral distribution φ _SSL (λ), the radiation efficiency K (Lu
minority of radiation (lm / W) followed the following widely used definition:

In the above formula,
K _m : Maximum visibility (lm / W)
V (λ): spectral luminous efficiency λ: wavelength (nm)
It is.

Test light when measuring light in the main radiation direction emitted from the light emitting device (according to the light emitting device of the present invention) or when measuring at the position of the illumination object (related to the illumination method of the present invention) The radiation efficiency K (lm / W) of the spectral distribution φ _SSL (λ) is the efficiency that the spectral distribution has as its shape, and the efficiency related to all the material characteristics that constitute the light emitting device (for example, the internal quantum efficiency of the semiconductor light emitting device) The light extraction efficiency, the internal quantum efficiency of the phosphor, the external quantum efficiency, and the efficiency of the light-transmitting property of the encapsulant) are 100%.

[Details of the second step]
As described above, as a second step, a luminaire that does not include a packaged LED light source and control elements was prototyped based on a mathematically examined spectrum (test light). In addition, a light source for light (experimental pseudo reference light) having _a high R _a and high R _i in which a color close to the calculation reference light appears, and a lighting fixture incorporating the light source were also prototyped.
Specifically, a green phosphor and a red phosphor are excited by a blue semiconductor light emitting device, a yellow phosphor and a red phosphor are excited by a blue semiconductor light emitting device, a blue phosphor and a green fluorescence are emitted by a purple semiconductor light emitting device. The light source which excited the body and the red phosphor was made as a prototype and made into an instrument.
BAM or SBCA was used as the blue phosphor. As the green phosphor, BSS, β-SiAlON, or BSON was used. YAG was used as the yellow phosphor. CASON or SCASN was used as the red phosphor.

  When making a package LED as a prototype, a commonly used method was used. Specifically, a semiconductor light emitting element (chip) was flip-chip mounted on a ceramic package in which a metal wiring capable of electrical conduction was contained. Next, the slurry which mixed the fluorescent substance and binder resin to be used was arrange | positioned as a fluorescent substance layer.

  After preparing the packaged LED, these were used to finish LED bulbs of MR16 Gu10 and MR16 Gu5.3. A driving circuit is built in the LED bulb, and a reflection mirror, a lens, and the like that are not affected by the intensity modulation with respect to the emission wavelength are mounted, and finished as one kind of lighting fixture. Some commercially available LED bulbs were also prepared. In addition, an incandescent bulb containing a tungsten filament was also prepared as a reference light for experiments.

In addition, a number of these LED bulbs were arranged to produce an illumination system for comparative visual experiments. Here, we have created a system that can instantly switch between three types of bulbs. One type of power supply line for driving is dedicated to incandescent bulbs (experimental reference light) having a tungsten filament, and a variable transformer is arranged at the subsequent stage to increase the driving voltage from 110 V to 130 V with respect to an input voltage of 100 V. As a result, the CCT can be changed.
Further, the remaining two systems of the drive power line are for LED bulbs, one of which is for experimental pseudo reference light (LED light source), and the other one is for test light.

[Details of the third step]
As a third step, a comparative visual experiment was performed in which the test light was switched by switching between the experimental reference light (or the experimental pseudo reference light) and the test light, and the subjects evaluated the appearance of the colors of many observation objects. The lighting system was installed in a dark room to eliminate disturbance. In addition, the illuminance at the position of the observation object was made substantially the same by changing the number of the experimental reference light (or experimental reference light) and test light mounted on the illumination system. The experiment was conducted in the range of about 150 lx to about 5000 lx.
Illustrated below are objects that are actually illuminated objects and observed objects. Here, consideration was given to preparing chromatic objects that cover all hues such as purple, blue-violet, blue, blue-green, green, yellow-green, yellow, yellow-red, red, and red-purple. Furthermore, achromatic objects such as white and black were also prepared. A lighting object having a color was prepared. Many kinds of still life, fresh flowers, food, clothing, printed matter, etc. were prepared. In the experiment, the subject's own skin was also observed. It should be noted that the color names partially appended before the object names below are not strict color representations in the sense that they look like that under normal circumstances.

White ceramic dish, white asparagus, white mushroom, white gerbera, white handkerchief, white Y-shirt, cooked rice, salted sesame, salt cracker purple fresh flower blue purple cloth handkerchief, blue jeans, blue green towel green paprika, lettuce, shredded cabbage, broccoli, green Lime, green apple yellow banana, yellow paprika, yellow green lemon, yellow gerbera, baked orange orange, orange paprika, carrot red tomato, red apple, red paprika, red wiener, plum dried pink tie, pink gerbera, salmon salt baked red bean tie, Beige work clothes, croquettes, tonkatsu, burdock, cookies, chocolate,
Peanuts, wooden test subjects (Japanese) own skin newspaper, color prints containing black letters on a white background (multicolored paper), paperback books, weekly magazine exterior wall color samples (Mitsubishi Resin Alpolic white, blue, green, yellow) ,Red)
Color checker (Color checker classic made by X-rite) Color chart of 24 colors including 18 chromatic colors and 6 achromatic colors (white 1, gray 4, black 1)
The names and Munsell notation of each color chart in the color checker are as follows.
Name Munsell Notation
Dark skin 3.05 YR 3.69 / 3.20
Light skin 2.2 YR 6.47 / 4.10
Blue sky 4.3 PB 4.95 / 5.55
Foliage 6.65 GY 4.19 / 4.15
Blue flower 9.65 PB 5.47 / 6.70
Bluish green 2.5 BG 7/6
Orange 5 YR 6/11
Purplish blue 7.5 PB 4 / 10.7
Moderate red 2.5 R 5/10
Purple 5 P 3/7
Yellow green 5 GY 7.08 / 9.1
Orange yellow 10 YR 7 / 10.5
Blue 7.5 PB 2.90 / 12.75
Green 0.1 G 5.38 / 9.65
Red 5 R 4/12
Yellow 5 Y 8 / 11.1
Magenta 2.5 RP 5/12
Cyan 5 B 5/8
White N 9.5 /
Neutral 8 N 8 /
Neutral 6.5 N 6.5 /
Neutral 5 N 5 /
Neutral 3.5 N 3.5 /
Black N 2 /

  In addition, it is not obvious that there is a correlation between the color appearance of various illumination objects used in the comparative visual experiment and the various mathematical indexes related to the color appearance of the 15 kinds of Munsell color charts used in the calculation. is not. This should be revealed through visual experiments.

The visual experiment was performed according to the following procedure.
Measure the light emitted in the main radiation direction of the prepared experimental reference light, experimental reference light, and test light, and each of them is measured for each CCT (related to the light-emitting device of the present invention) or for the prepared experimental light The reference light, the experimental pseudo reference light, and the test light were classified into six experiments for each CCT measured at the position of the illumination object (according to the illumination method of the present invention). That is, it is as follows.

  In one visual experiment, the same object is illuminated by switching between experimental reference light (or experimental pseudo-reference light) and test light, and each light is natural and lively as seen outdoors. The subjects were asked to make a relative judgment as to whether high visibility and comfortable color appearance and object appearance could be realized. At that time, he asked why he was superior or inferior.

[Fourth step details Experimental results]
In the fourth step, the results of the comparative visual experiment conducted in the third step were summarized using the LED light source / apparatus / system that was prototyped in the second step and did not include a control element. Table 2 corresponds to Experiment A, and Table 3 is the result corresponding to Experiment B. Similarly, Table 7 shows the results corresponding to Experiment F. In Tables 2 to 7, the overall evaluation of the test light with respect to the reference light is centered on “0” indicating the same degree of appearance, the evaluation that the test light is slightly preferable is “1”, and the evaluation that the test light is preferable is “2”, evaluation that test light is more preferable is “3”, evaluation that test light is very preferable is “4”, and evaluation that test light is extremely preferable is “5”. On the other hand, the evaluation that test light is slightly unfavorable is “−1”, the evaluation that test light is not preferable is “−2”, the evaluation that test light is not preferable is “−3”, and the test light is very Is evaluated as “−4”, and the evaluation that the test light is not particularly preferable is defined as “−5”.

、
ΔＣ_ｎ、（ΔＣ_ｍａｘ−ΔＣ_ｍｉｎ）を指標としてまとめた。なお、｜Δｈ_ｎ｜、ΔＣ_ｎは、ｎを選択すると値が変化するが、ここでは最大値と最小値を示した。これらの値も表２から表７に合わせて記載した。なお、照明対象物の色の見えに関して、発光装置から出射された主たる放射方向の試験光（本発明の発光装置に係る）、又は、被験者の総合的評価結果が照明対象物の位置における試験光（本発明の照明方法に係る）のＤ_ｕｖ値に比較的依存していたので、表２から表７は、Ｄ_ｕｖの値が低下する順に並べた。
全体としては、本実験によって、Ｄ_ｕｖが適切な値で負の値をとり、かつ、指標Ａ_ｃｇ等が適切な範囲にある場合に、又は、｜Δｈ_ｎ｜、

、
ΔＣ_ｎ、（ΔＣ_ｍａｘ−ΔＣ_ｍｉｎ）等が適切な範囲にある場合に、試験光で照明していた実観察物の物体の見え、色の見えは、実験用基準光で照明した場合よりも好ましいと判断された。これはステップ１で「現在広く信じられている常識に照らした結果」に対して予想外であった。
In the fourth step, in particular, in visual experiments, it was determined that the color appearance of the illumination object when illuminated with test light was better than when illuminated with experimental reference light or experimental reference light. In some cases, we tried to extract the radiometric and photometric characteristics of the spectral distribution common to the test light from the measured spectrum. That is, with respect to numerical values such as A _cg , radiation efficiency K (lm / W), CCT (K), and D _uv , the light emitted from the light emitting device in the main radiation direction (related to the light emitting device of the present invention) and the illumination target The characteristics of the position of the object (related to the lighting method of the present invention) were extracted. At the same time, the color appearance of the 15 color chart assuming the case where it is illuminated with the calculation reference light and the test light spectral distribution obtained by actually measuring the light emitted from the light emitting device in the main radiation direction (related to the light emitting device of the present invention) Also, regarding the difference between the appearances of the colors of the 15 color chart assuming that the illumination is performed with the test light spectral distribution (according to the illumination method of the present invention) measured at the position of the illumination object, | Δh _n | ,

,
ΔC _n and (ΔC _max −ΔC _min ) were collected as indices. The values of | Δh _n | and ΔC _n change when n is selected, but the maximum value and the minimum value are shown here. These values are also shown in Tables 2 to 7. Regarding the color appearance of the illumination object, the test light in the main radiation direction emitted from the light-emitting device (related to the light-emitting device of the present invention) or the test light at the position of the illumination object is a comprehensive evaluation result of the subject. Since it was relatively dependent on the D _uv value (according to the illumination method of the present invention), Tables 2 to 7 are arranged in order of decreasing D _uv value.
As a whole, according to this experiment, when D _uv is an appropriate value and takes a negative value, and the index A _cg or the like is in an appropriate range, or | Δh _n |,

,
When ΔC _n , (ΔC _max −ΔC _min ), etc. are in an appropriate range, the appearance and color appearance of the actual observation object illuminated with the test light is more than that when illuminated with the experimental reference light. It was judged preferable. This was unexpected for Step 1 “results in light of common sense now widely believed”.

[Detailed discussion on the fourth step]
The experimental results are considered below. The test light and comparative test light in the table may be collectively referred to as “test light”.
1) When the D _{uv of the} test light is on the positive side of the experimental reference light (or the pseudo reference light for the experiment) Tables 4, 5, and 7 show that the D _{uv of} the test light is the experimental reference light. The result on the positive side of the light (or the pseudo reference light for experiment) is included. From this, it can be seen that the more the test light D _uv becomes positive, the more the subject is judged to be unfavorable regarding the color appearance of the illumination object and the appearance of the object. Specifically, it was as follows.

The subject judged that the appearance of the illuminated white object appeared more yellowish (greenish) as D _uv became more positive, and the sense of discomfort increased. The subject judged that the gray portion of the illuminated color checker was less visible due to the difference in brightness. In addition, the subject pointed out that the letters on the illuminated printed material became more difficult to see. Furthermore, the appearance of various illuminated chromatic colors becomes more unnatural as the D _{uv of} the test light becomes more positive as compared to the case of illumination with the experimental reference light (or the experimental pseudo reference light). The subject judged it looked dull. The subjects pointed out that the various color samples of the exterior wall materials that were illuminated were perceived very different from the color appearance seen outdoors, and that their skin color also looked unnatural and unhealthy. In addition, the subject pointed out that the color difference of the same kind of similar color petals was harder to identify and the contour was harder to see than when illuminated with experimental reference light.

In addition, these results do not depend very much on the CCT of the test light described in Table 4, Table 5, and Table 7, and also do not depend much on the configuration of the light emitting element (light emitting material) of the light emitting device. It was.
As the test light D _uv becomes more positive, Ra decreases as an overall trend. Therefore, it can be said that some of these results were within a range that could be predicted from the detailed mathematical examination in Step 1.

2) When the D _{uv of the} test light is more negative than the experimental reference light (or the experimental pseudo reference light) All of Tables 2 to 7 show that the D _{uv of} the test light is the experimental reference light ( Alternatively, a result on the negative side of the experimental pseudo-reference light) is included. According to these, when the D _{uv of} the test light is negative in the appropriate range and the various indicators in the table are in the appropriate range, the subject It turns out that it was judged that it was slightly preferable, preferable, more preferable, very preferable, and extremely preferable. On the other hand, even if the D _{uv of} the test light is negative in the same range, when the various indicators in the table are not in the appropriate range, as shown in Table 5, the color appearance and the object by the test light It can also be seen that the appearance was judged unfavorable.

Here, when the D _uv of the test light is negative in the proper range and the various indicators in the table are in the proper range, the appearance of the color of the object when illuminated with the test light is an experimental reference. Compared to the case of illuminating with light (or experimental pseudo-reference light), it was completely unexpected that natural and preferable color appearances and preferable object appearances were obtained. Details of the features pointed out by the subjects were as follows.

For white objects, when the D _{uv of} the test light is negative within the appropriate range and the various indicators in the table are within the appropriate range, the white light is compared with the case where the test light is illuminated with the experimental reference light (or experimental pseudo reference light). The subject judged that the yellowishness (greenishness) was reduced, it looked slightly white, looked white, looked whiter, looked very white, and looked much whiter. He also pointed out that the closer to the optimum range, the more natural and better it looked. This was a completely unexpected result.
Further, the gray portion of the color checker is illuminated with experimental reference light (or experimental pseudo reference light) when the D _{uv of} the test light is negative within the appropriate range and the various indicators in the table are within the appropriate range. Compared to the case, the difference in brightness seemed to be slightly increased, seemed to be increased, seemed to be increased, seemed to be greatly increased, and seemed to be greatly increased. The subject determined that it was visible. The subjects also noted that as they approached the optimal range, they looked more natural and more visible. This was a completely unexpected result.

Further, the outline of each achromatic color chart also has an experimental reference light (or an experimental pseudo reference light) when the D _{uv of} the test light is negative in the appropriate range and the various indicators in the table are in the appropriate range. The subject judged that it was slightly clearer, more clearly visible, more clearly visible, very clearly visible, and much more clearly visible than when illuminated in (). The subjects also noted that as they approached the optimal range, they looked more natural and more visible. This was a completely unexpected result.
Further, the print characters, in the negative in D _uv is proper range of the test light, and, in the case various indices in the table is in the proper range, when illuminated by a laboratory reference light (or experimental pseudo reference light) The subjects judged that it was slightly easier to see, easier to see, easier to see, much easier to see, and much easier to see. The subjects also pointed out that as they approached the optimum range, the characters became more natural and more visible. This was a completely unexpected result.

In addition, the color appearance of various chromatic colored illumination objects is determined when the test light D _uv is negative within the appropriate range and the various indicators in the table are within the appropriate range. Compared to the case of illuminating with (pseudo-reference light), it was a natural vividness that was a little, but a natural vividness, a more natural vividness, a very natural vividness. In addition, the subject judged that it was remarkably natural vividness. The subjects also pointed out that as they approached the optimal range, they became more natural and preferred in appearance. This was a completely unexpected result.
Furthermore, the color appearance of the various color samples of the outer wall material is such that when the D _{uv of} the test light is negative in the proper range and the various indicators in the table are in the proper range, the experimental reference light (or the experimental pseudo reference) Compared to the case of illuminating with light), when viewed outdoors, it was slightly closer, was closer, was closer, was very close, and was much closer The subject judged that he was. The subjects also pointed out that as they approached the optimal range, they became more natural and looked like a favorable color closer to memory when viewed outdoors. This was a completely unexpected result.

Furthermore, the appearance of the skin color of the subject himself (Japanese) is the reference light for experiment (or experiment) when the D _{uv of} the test light is negative within the proper range and the various indicators in the table are within the proper range. The subject judged that it looked somewhat natural, looked natural, looked more natural, looked very natural, and looked much more natural than when illuminated with a pseudo-standard light. . The subjects also pointed out that as they approached the optimum range, they became more natural and healthy in appearance. This was a completely unexpected result.
Furthermore, the color difference of the same kind and similar colors of the flower petals is that the test light D _uv is negative in the appropriate range and the various indicators in the table are in the appropriate range. The subjects judged that it was slightly easier to identify, easier to identify, easier to identify, very easy to identify, and much easier to identify than when illuminated in (1). In addition, the test subject pointed out that the more the D _uv became negative than the appropriate upper limit within the experimented range, the easier it was to identify. This was a completely unexpected result.

Further, various illumination objects were illuminated with the experimental reference light (or experimental pseudo reference light) when the D _{uv of} the test light was negative within the appropriate range and the various indicators in the table were within the appropriate range. Compared to the case, the subject judged that the outline was slightly clear, the outline was clearly visible, the outline was more clearly visible, the outline was very clearly visible, and the outline was clearly visible. In addition, the test subject pointed out that the outline became clearer as D _uv became negative from the appropriate upper limit within the experimental range. This was a completely unexpected result.

From the mathematical detailed examination of Step 1, it can be said that these results are completely unexpected because Ra becomes lower as a general tendency as the D _{uv of the} test light becomes negative. As shown in Tables 2 to 7, if attention is paid only to the value of Ra, for example, there are many test lights with Ra of 95 or more. The Ra was about 82 to 91. In addition, this comparative visual experiment was conducted beyond the range of D _uv described in ANSI C78.377-2008. Therefore, it can be said that the above result is a new finding that there is a perceptual good region regarding the color appearance of the illuminated object outside the current common sense recommended chromaticity range.

、
ΔＣ_ｎ、（ΔＣ_ｍａｘ−ΔＣ_ｍｉｎ）、が適正範囲にあることが好ましいことが解った。 In the light emitting device according to the first embodiment of the present invention, in order to obtain such a perception, it is necessary that the index A _cg described in Tables 2 to 7 is within an appropriate range in addition to D _uv . Further, various indexes, that is, radiation efficiency K (lm / W), | Δh _n |,

,
It has been found that ΔC _n and (ΔC _max −ΔC _min ) are preferably in an appropriate range.

First, from the result of the test light judged to be good in the visual experiment, the D _uv and the index A _cg were as follows.

First, the D _uv value is −0.0040 or less, slightly preferably −0.0042 or less, preferably −0.0070 or less, more preferably −0.0100 or less. It was very preferably −0.0120 or less, and particularly preferably −0.0160 or less.
Further, D _uv in the present invention is −0.0350 or more, slightly preferably −0.0340 or more, preferably −0.0290 or more, more preferably −0.0250 or more. And, it was very preferably −0.0230 or more, and particularly preferably −0.0200 or more.

Furthermore, from the results of Table 2 to Table 7, in the light emitting device according to the first embodiment of the present invention, the spectral distribution was A _cg of −10 or less and −360 or more. The exact definition is as described above, but the approximate physical meaning and good interpretation are as follows. The meaning that A _cg takes a negative value in an appropriate range means that there is an appropriate unevenness in the standardized test light spectral distribution, and in the short wavelength region between 380 nm and 495 nm, the mathematical standardized reference light spectral distribution is Tends to have a higher radiant flux intensity of the normalized test light spectral distribution and / or in the intermediate wavelength region from 495 nm to 590 nm, the radiant flux of the normalized test light spectral distribution than the mathematical standardized reference light spectral distribution. Means that the intensity tends to be weak and / or, in the long wavelength region from 590 nm to Λ4, the radiant flux intensity of the normalized test light spectral distribution tends to be stronger than the mathematical standardized reference light spectral distribution. doing. In addition, it can be understood that when A _cg is quantitatively −10 or less and −360 or more, a good color appearance and a good object appearance are obtained.

A _cg derived from the spectral distribution of the light emitted in the main radiation direction from the light emitting device according to the first embodiment of the present invention is −10 or less, more preferably −11 or less, and more It was preferably −28 or less, very preferably −41 or less, and particularly preferably −114 or less.
Further, A _cg derived from the spectral distribution of the light emitted in the main radiation direction from the light emitting device according to the first embodiment of the present invention is −360 or more, and is preferably −330 or more, It was preferably -260 or more, very preferably -181 or more, and particularly preferably -178 or more.
Incidentally, consider using real test light in the visual experiments have been made, the preferable range of A _cg inside the preferred experimental results in the study, -322 or higher, was -12.

Secondly, the present invention aimed to realize test light with good color appearance and high efficiency, and the radiation efficiency K was as follows.
The radiation efficiency of the spectral distribution of the light emitting device according to the first embodiment of the present invention is preferably in the range of 180 (lm / W) to 320 (lm / W), and is a value of a normal incandescent bulb or the like. Was at least 20% higher than 150 (lm / W). This is presumably because radiation from the semiconductor light-emitting element and radiation from the phosphor are inherent, and there are appropriate irregularities at appropriate positions in the spectral distribution in relation to V (λ). From the standpoint of compatibility with color appearance, the following range is preferable for the radiation efficiency obtained from the spectral distribution of the light emitted in the main radiation direction from the light emitting device according to the first embodiment of the present invention. It was.

The radiation efficiency K of the light emitting device according to the first embodiment of the present invention is preferably 180 (lm / W) or more, but is preferably 205 (lm / W) or more, preferably 208. (Lm / W) or more, and very preferably 215 (lm / W) or more. On the other hand, the radiation efficiency K is ideally high, but in the present invention, it is preferably 320 (lm / W) or less, and 282 (lm / W) or less from the balance with the color appearance. Is slightly preferred, preferably 232 (lm / W) or less, and particularly preferably 231 (lm / W) or less.
In addition, the examination using the actual test light was made in the visual experiment, and the preferable range of K inside the preferable experiment result under the examination was 206 (lm / W) or more and 288 (lm / W) or less. .

、
ΔＣ_ｎ、（ΔＣ_ｍａｘ−ΔＣ_ｍｉｎ）の特性を考えると、以下の傾向であったことが分かる。すなわち、良好な色の見え、物体の見えとなる試験光は、計算用基準光で照明した場合を仮定した当該１５色票の色の見えと、実測した試験光分光分布で照明した場合を仮定した当該１５色票の色の見えに関して、以下の特性を有していた。 Third, | Δh _n |,

,
Considering the characteristics of ΔC _n and (ΔC _max −ΔC _min ), it can be seen that the following tendency was observed. That is, the test light that gives good color appearance and object appearance is assumed to be the color appearance of the 15-color chart assumed when illuminated with the reference light for calculation, and the illumination with the measured test light spectral distribution. The color appearance of the 15 color chart had the following characteristics.

が、計算用基準光による照明のそれと比較して適正な範囲で上がっていた。かつ、当該平均値だけでなく、１５色票の飽和度（ΔＣ_ｎ）を個別に見ても、試験光による照明の当該１５色票の各ΔＣ_ｎが、計算用基準光による照明のそれらと比較して、極端に低下しているものも極端に向上しているものもなく、すべてが適正範囲にあり、この結果として最大最小飽和度差間差（ΔＣ_ｍａｘ−ΔＣ_ｍｉｎ）が適正な範囲で狭かった。さらに、簡略化すれば、当該１５色票に対して基準光での照明を仮定した場合に比較して、試験光での照明を仮定した場合は、当該１５色票すべての色相において、色相角差が少なく、かつ、適正な範囲で１５色票の飽和度が比較的均等に向上している場合が理想的であると推察できる。 The hue angle difference (| Δh _n |) of the 15 color chart between the illumination by the test light and the illumination by the calculation reference light is relatively small, and the average saturation of the 15 color chart of the illumination by the test light

However, it was higher in the proper range than that of the illumination with the reference light for calculation. In addition, not only the average value but also the saturation (ΔC _n ) of the 15 color charts, each ΔC _{n of the} 15 color charts of the illumination by the test light is different from those of the illumination by the reference light for calculation. In comparison, there is neither extremely decreased nor extremely improved, all are in the appropriate range, and as a result, the difference between the maximum and minimum saturation differences (ΔC _max −ΔC _min ) is in the appropriate range. It was narrow. Furthermore, in a simplified manner, when the illumination with the test light is assumed as compared with the case where the illumination with the reference light is assumed for the 15 color chart, the hue angle in all the hues of the 15 color chart is assumed. It can be inferred that the difference is small and the saturation of the 15 color charts is improved relatively evenly in an appropriate range.

The solid line in FIG. 35 is a normalized test light spectral distribution of the test light 5 that is determined in Table 3 to be “remarkably preferable” as a comprehensive judgment. Also, the dotted line in the figure is the normalized spectral distribution of the calculation reference light (black body radiation light) calculated from the CCT of the test light. On the other hand, FIG. 36 relates to the appearance of the color of the 15 color chart, assuming the case of illumination with the test light 5 (solid line) and the case of illumination with the reference light for calculation (light of black body radiation) (dotted line). CIELAB plot. In addition, although the vertical direction on the paper is lightness, only the a ^* and b ^* axes are plotted here for convenience.
Further, FIGS. 37 and 38 summarize the results of the test light 15 determined as “remarkably preferable” as the overall determination in Table 5 in the same manner as described above. FIGS. Among them, the results of the test light 19 determined as “remarkably preferable” as a comprehensive determination are summarized in the same manner as described above.

  In this way, when a favorable color appearance and an object appearance are obtained in the visual experiment, when the illumination with the test light is assumed as compared with the case where the illumination with the reference light for the 15 color chart is assumed, It can be seen that, in all hues of the 15 color charts, the hue angle difference is small and the saturation of the 15 color charts is improved relatively evenly in an appropriate range. It can also be seen from this point of view that a CCT near 4000K is preferable.

On the other hand, even if D _uv has a negative value in an appropriate range, for example, in the case of the comparative test light 14 in Table 5 where D _uv ≈−0.08331, the visual test results in the appearance by the test light. Is determined to be undesirable. This is considered that the characteristic of the index A _cg was not appropriate. 41 and 42 show the results of performing CIELAB plots on the comparative test light 14 in the same way as in FIGS. 35 and 36, etc., regarding the normalized spectral distribution and the color appearance of the 15 color chart. As is apparent from this figure, when the illumination with the reference light is assumed for the 15 color chart and the illumination with the test light is assumed, several hues of the 15 color chart are compared. It can be seen that the difference in hue angle is large and the saturation of the 15 color charts varies very unevenly.

From the results of visual experiment and consideration, it can be seen that the following ranges are preferable for each quantitative index.
As described above, D _uv in the light emitting device according to the first embodiment of the present invention is −0.0040 or less, slightly preferably −0.0042 or less, and preferably −0.0070 or less. More preferably, it was −0.0100 or less, very preferably −0.0120 or less, and particularly preferably −0.0160 or less.
Further, D _uv in the light emitting device according to the first embodiment of the present invention is −0.0350 or more, slightly preferably −0.0340 or more, and preferably −0.0290 or more. More preferably, it was -0.0250 or more, very preferably -0.0230 or more, and particularly preferably -0.0200 or more.

In the light emitting device according to the first embodiment of the present invention, | Δh _n | is preferably 9.0 or less, very preferably 8.4 or less, and particularly preferably 7.3 or less. . Further, | Δh _n | is considered to be even smaller, more preferably 6.0 or less, still more preferably 5.0 or less, and particularly preferably 4.0 or less.
In the light emitting device according to the first embodiment of the present invention, | Δh _n | is preferably 0 or more, and the minimum value during the visual experiment is 0.0029. Furthermore, examination using actual test light was performed in a visual experiment, and a preferable range of | Δh _n | inside a preferable experimental result under examination was 8.3 or less and 0.003 or more.

は、１．０以上が好適であり、若干好ましくは１．１以上であって、好ましくは、１．９以上であって、非常に好ましくは２．３以上であって、格段に好ましくは２．６以上であった。
また、７．０以下であることが好適であり、好ましくは６．４以下であって、非常に好ましくは、５．１以下であって、格段に好ましくは４．７以下であった。
なお、視覚実験で実試験光を用いた検討がなされ、当該検討中の好ましい実験結果の内側にある上記指標の好ましい範囲は、１．２以上、６．３以下であった。 In the light emitting device according to the first embodiment of the present invention.

Is preferably 1.0 or more, slightly preferably 1.1 or more, preferably 1.9 or more, very preferably 2.3 or more, and particularly preferably 2 .6 or more.
Also, it is preferably 7.0 or less, preferably 6.4 or less, very preferably 5.1 or less, and particularly preferably 4.7 or less.
In addition, the examination using the actual test light was made in the visual experiment, and the preferred range of the above index inside the preferred experimental result under the examination was 1.2 or more and 6.3 or less.

ΔC _n in the light emitting device according to the first embodiment of the present invention is preferably −3.8 or more, slightly preferably −3.5 or more, and very preferably −2. It was 5 or more, and particularly preferably -0.7 or more.
In addition, ΔC _n in the light emitting device according to the first embodiment of the present invention is preferably 18.6 or less, very preferably 17.0 or less, and particularly preferably 15. 0 or less.
In addition, the examination using the actual test light was made in the visual experiment, and the preferable range of ΔC _n inside the preferable experimental result under the examination was −3.4 or more and 16.8 or less.

(ΔC _max −ΔC _min ) in the light emitting device according to the first embodiment of the present invention is preferably 19.6 or less, very preferably 17.9 or less, and 15.2 or less. It was much better to be. In addition, it is considered more preferable that (ΔC _max −ΔC _min ) is small, 14.0 or less is more preferable, and 13.0 or less is considered extremely preferable.
Further, (ΔC _max −ΔC _min ) in the light emitting device according to the first embodiment of the present invention is preferably 2.8 or more, and the minimum value during the visual experiment was 3.16. Furthermore, the examination using the actual test light was made in the visual experiment, and the preferred range of (ΔC _max −ΔC _min ) inside the preferred experimental result under consideration was 3.2 or more and 17.8 or less. .

、
ΔＣ_ｎ、（ΔＣ_ｍａｘ−ΔＣ_ｍｉｎ）をより適切な値とするためには、本発明の第一の実施態様に係る発光装置において、ＣＣＴは４０００Ｋに近い値をとることが好ましかった。これは４０００Ｋ付近の光は基準の光を見てもその分光分布が波長にあまり依存せずに等エネルギー的であって、基準の光に対して容易に凹凸を形成した試験光分光分布が実現できるためと考えられる。換言すると、他のＣＣＴの場合と比較しても、｜Δｈ_ｎ｜と（ΔＣ_ｍａｘ−ΔＣ_ｍｉｎ）を比較的小さく保持したまま、

を増加させ、大多数の色票に対するΔＣ_ｎを所望の値に容易に制御可能である。 Fourthly, the following has been found regarding CCT in the light emitting device according to the first embodiment of the present invention. Various indexes determined to be preferable by comparative visual experiments, that is, | Δh _n |,

,
In order to set ΔC _n and (ΔC _max −ΔC _min ) to a more appropriate value, it is preferable that the CCT take a value close to 4000 K in the light emitting device according to the first embodiment of the present invention. This is because the spectral distribution of light around 4000K is isoenergetic regardless of the wavelength even if the reference light is viewed, and a test light spectral distribution in which irregularities are easily formed with respect to the reference light is realized. This is thought to be possible. In other words, | Δh _n | and (ΔC _max −ΔC _min ) are kept relatively small as compared with other CCT cases.

And ΔC _n for the majority of color charts can be easily controlled to a desired value.

Therefore, the CCT in the light emitting device according to the first embodiment of the present invention is slightly preferably from 1800K to 15000K, more preferably from 2000K to 10,000K, more preferably from 2300K to 7000K, and from 2600K to 6600K. It is very particularly preferred that it is 2900K to 5800K, and most preferred is 3400K to 5100K.
In addition, the examination using the actual test light was made in the visual experiment, and the preferable range of CCT inside the preferable experimental result under the examination was 2550 (K) or more and 5650 (K) or less.

、
ΔＣ_ｎ、（ΔＣ_ｍａｘ−ΔＣ_ｍｉｎ）が適正範囲にある必要があった。また、指標Ａ_ｃｇ、放射効率Ｋ（ｌｍ／Ｗ）が適正範囲にあることが好ましいことが解った。 In addition, in the illumination method according to the third embodiment of the present invention, in order to obtain such perception, in addition to D _uv , various indexes described in Tables 2 to 7, that is, | Δh _n |,

,
ΔC _n , (ΔC _max −ΔC _min ) needs to be in an appropriate range. It was also found that the index A _cg and the radiation efficiency K (lm / W) are preferably in the appropriate ranges.

、
ΔＣ_ｎ、（ΔＣ_ｍａｘ−ΔＣ_ｍｉｎ）の特性を考えると、以下の傾向であったことが分かる。すなわち、良好な色の見え、物体の見えとなる試験光は、計算用基準光で照明した場合を仮定した当該１５色票の色の見えと、実測した試験光分光分布で照明した場合を仮定した当該１５色票の色の見えに関して、以下の特性を有していた。 In particular, from the result of the test light determined to be good in the visual experiment, | Δh _n |,

,
Considering the characteristics of ΔC _n and (ΔC _max −ΔC _min ), it can be seen that the following tendency was observed. That is, the test light that gives good color appearance and object appearance is assumed to be the color appearance of the 15-color chart assumed when illuminated with the reference light for calculation, and the illumination with the measured test light spectral distribution. The color appearance of the 15 color chart had the following characteristics.

が、計算用基準光による照明のそれと比較して適正な範囲で上がっていた。かつ、当該平均値だけでなく、１５色票の飽和度（ΔＣ_ｎ）を個別に見ても、試験光による照明の当該１５色票の各ΔＣ_ｎが、計算用基準光による照明のそれらと比較して、極端に低下しているものも極端に向上しているものもなく、すべてが適正範囲にあり、この結果として最大最小飽和度差間差（ΔＣ_ｍａｘ−ΔＣ_ｍｉｎ）が適正な範囲で狭かった。さらに、簡略化すれば、当該１５色票に対して基準光での照明を仮定した場合に比較して、試験光での照明を仮定した場合は、当該１５色票すべての色相において、色相角差が少なく、かつ、適正な範囲で１５色票の飽和度が比較的均等に向上している場合が理想的であると推察できる。 The hue angle difference (| Δh _n |) of the 15 color chart between the illumination by the test light and the illumination by the calculation reference light is relatively small, and the average saturation of the 15 color chart of the illumination by the test light

However, it was higher in the proper range than that of the illumination with the reference light for calculation. In addition, not only the average value but also the saturation (ΔC _n ) of the 15 color charts, each ΔC _{n of the} 15 color charts of the illumination by the test light is different from those of the illumination by the reference light for calculation. In comparison, there is neither extremely decreased nor extremely improved, all are in the appropriate range, and as a result, the difference between the maximum and minimum saturation differences (ΔC _max −ΔC _min ) is in the appropriate range. It was narrow. Furthermore, in a simplified manner, when the illumination with the test light is assumed as compared with the case where the illumination with the reference light is assumed for the 15 color chart, the hue angle in all the hues of the 15 color chart is assumed. It can be inferred that the difference is small and the saturation of the 15 color charts is improved relatively evenly in an appropriate range.

The solid line in FIG. 35 is a normalized test light spectral distribution of the test light 5 that is determined in Table 3 to be “remarkably preferable” as a comprehensive judgment. Also, the dotted line in the figure is the normalized spectral distribution of the calculation reference light (black body radiation light) calculated from the CCT of the test light. On the other hand, FIG. 36 relates to the appearance of the color of the 15 color chart, assuming the case of illumination with the test light 5 (solid line) and the case of illumination with the reference light for calculation (light of black body radiation) (dotted line). CIELAB plot. In addition, although the vertical direction on the paper is lightness, only the a ^* and b ^* axes are plotted here for convenience.
Further, FIGS. 37 and 38 summarize the results of the test light 15 determined as “remarkably preferable” as the overall determination in Table 5 in the same manner as described above. FIGS. Among them, the results of the test light 19 determined as “remarkably preferable” as a comprehensive determination are summarized in the same manner as described above.

  In this way, when a favorable color appearance and an object appearance are obtained in the visual experiment, when the illumination with the test light is assumed as compared with the case where the illumination with the reference light for the 15 color chart is assumed, It can be seen that, in all hues of the 15 color charts, the hue angle difference is small and the saturation of the 15 color charts is improved relatively evenly in an appropriate range. It can also be seen from this point of view that a CCT near 4000K is preferable.

、
ΔＣ_ｎ、（ΔＣ_ｍａｘ−ΔＣ_ｍｉｎ）の特性のうちいくつかが適正でなかったと考えられる。図４１、図４２は比較試験光１４について、図３５、図３６等と同様に規格化分光分布と１５色票の色の見えに関するＣＩＥＬＡＢプロットを行った結果である。この図からも明らかなように、当該１５色票に対して基準光での照明を仮定した場合と、試験光での照明を仮定した場合とを比較すると、当該１５色票のいくつかの色相において、色相角差がおおきく、また、１５色票の飽和度が非常に不均等に変化していることが分かる。 On the other hand, even if D _uv has a negative value in an appropriate range, for example, in the case of the comparative test light 14 in Table 5 where D _uv ≈−0.08331, the visual test results in the appearance by the test light. Is determined to be undesirable. This is | Δh _n |,

,
It is considered that some of the characteristics of ΔC _n and (ΔC _max −ΔC _min ) were not appropriate. 41 and 42 show the results of performing CIELAB plots on the comparative test light 14 in the same way as in FIGS. 35 and 36, etc., regarding the normalized spectral distribution and the color appearance of the 15 color chart. As is apparent from this figure, when the illumination with the reference light is assumed for the 15 color chart and the illumination with the test light is assumed, several hues of the 15 color chart are compared. It can be seen that the difference in hue angle is large and the saturation of the 15 color charts varies very unevenly.

From the results of visual experiment and consideration, it can be seen that the following ranges are preferable for each quantitative index.
The D _uv in the illumination method according to the third embodiment of the present invention is −0.0040 or less, slightly preferably −0.0042 or less, preferably −0.0070 or less, More preferably, it was −0.0100 or less, very preferably −0.0120 or less, and particularly preferably −0.0160 or less.
In addition, D _uv in the illumination method according to the third embodiment of the present invention is −0.0350 or more, slightly preferably −0.0340 or more, and preferably −0.0290 or more. More preferably, it is -0.0250 or more, and very preferably -0.02
It was 30 or more, and particularly preferably −0.0200 or more.

In the illumination method according to the third embodiment of the present invention, | Δh _n | is 9.0 or less, very preferably 8.4 or less, and particularly preferably 7.3 or less. Further, | Δh _n | is considered to be even smaller, more preferably 6.0 or less, still more preferably 5.0 or less, and particularly preferably 4.0 or less.
In the illumination method according to the third embodiment of the present invention, | Δh _n | was 0 or more, and the minimum value during the visual experiment was 0.0029. Furthermore, examination using actual test light was performed in a visual experiment, and a preferable range of | Δh _n | inside a preferable experimental result under examination was 8.3 or less and 0.003 or more.

は、１．０以上であって、若干好ましくは１．１以上であって、好ましくは、１．９以上であって、非常に好ましくは２．３以上であって、格段に好ましくは２．６以上であった。
また、７．０以下であって、好ましくは６．４以下であって、非常に好ましくは、５．１以下であって、格段に好ましくは４．７以下であった。
なお、視覚実験で実試験光を用いた検討がなされ、当該検討中の好ましい実験結果の内側にある上記指標の好ましい範囲は、１．２以上、６．３以下であった。 In the illumination method according to the third embodiment of the present invention.

Is 1.0 or more, slightly preferably 1.1 or more, preferably 1.9 or more, very preferably 2.3 or more, and particularly preferably 2. It was 6 or more.
Moreover, it was 7.0 or less, Preferably it was 6.4 or less, Very preferably, it was 5.1 or less, Most preferably, it was 4.7 or less.
In addition, the examination using the actual test light was made in the visual experiment, and the preferred range of the above index inside the preferred experimental result under the examination was 1.2 or more and 6.3 or less.

ΔC _n in the illumination method according to the third embodiment of the present invention is −3.8 or higher, slightly preferably −3.5 or higher, and very preferably −2.5 or higher. Especially preferably, it was -0.7 or more.
In addition, ΔC _n in the illumination method according to the third embodiment of the present invention is 18.6 or less, very preferably 17.0 or less, and particularly preferably 15.0 or less. . Furthermore, examination using actual test light was performed in a visual experiment, and a preferable range of ΔC _n inside a preferable experimental result under examination was −3.4 or more and 16.8 or less.

In the illumination method according to the third embodiment of the present invention, (ΔC _max −ΔC _min ) is 19.6 or less, but is very preferably 17.9 or less, and is 15.2 or less. It was much better. In addition, it is considered more preferable that (ΔC _max −ΔC _min ) is small, 14.0 or less is more preferable, and 13.0 or less is considered extremely preferable.
Further, (ΔC _max −ΔC _min ) in the illumination method according to the third embodiment of the present invention was 2.8 or more, and the minimum value during the visual experiment was 3.16. Furthermore, the examination using the actual test light was made in the visual experiment, and the preferred range of (ΔC _max −ΔC _min ) inside the preferred experimental result under consideration was 3.2 or more and 17.8 or less. .

  On the other hand, using Tables 2 to 7, the characteristics associated with the test light comprehensively judged to be favorable characteristics in the visual experiment are represented by the radiometric characteristics and the photometric characteristics of the test light spectral distribution. I tried to make it.

Also in this case, the D _uv value is as discussed above, and is −0.0040 or less, preferably slightly −0.0042 or less, and preferably −0.0070 or less. More preferably, it was −0.0100 or less, very preferably −0.0120 or less, and particularly preferably −0.0160 or less.
Further, D _uv in the present invention is −0.0350 or more, slightly preferably −0.0340 or more, preferably −0.0290 or more, more preferably −0.0250 or more. And, it was very preferably −0.0230 or more, and particularly preferably −0.0200 or more.

On the other hand, the index A _cg was as follows.
From the results of Tables 2 to 7, the preferred spectral distribution of the illumination method according to the third embodiment of the present invention was A _cg of −10 or less and −360 or more. The exact definition is as described above, but the approximate physical meaning and good interpretation are as follows. The meaning that A _cg takes a negative value in an appropriate range means that there is an appropriate unevenness in the standardized test light spectral distribution, and in the short wavelength region between 380 nm and 495 nm, the mathematical standardized reference light spectral distribution is Tends to have a higher radiant flux intensity of the normalized test light spectral distribution and / or in the intermediate wavelength region from 495 nm to 590 nm, the radiant flux of the normalized test light spectral distribution than the mathematical standardized reference light spectral distribution. Means that the intensity tends to be weak and / or, in the long wavelength region from 590 nm to Λ4, the radiant flux intensity of the normalized test light spectral distribution tends to be stronger than the mathematical standardized reference light spectral distribution. doing. Since A _cg is the sum of the respective elements in the short wavelength region, the intermediate wavelength region, and the long wavelength region, each individual element may not necessarily have the above tendency. In addition, it can be understood that when A _cg is quantitatively −10 or less and −360 or more, a good color appearance and a good object appearance are obtained.

A _cg in the lighting method according to the third embodiment of the present invention is preferably −10 or less, slightly preferably −11 or less, more preferably −28 or less, and very preferably. Was −41 or less, and particularly preferably −114 or less.
In the illumination method according to the third embodiment of the present invention, A _cg is preferably −360 or more, slightly preferably −330 or more, preferably −260 or more, It was preferably -181 or more, and particularly preferably -178 or more.
Incidentally, consider using real test light in the visual experiments have been made, the preferable range of A _cg inside the preferred experimental results in the study, -322 or higher, was -12.

Furthermore, in the illumination method according to the third embodiment of the present invention, it was aimed to realize test light with good color appearance and high efficiency, but the radiation efficiency K was as follows.
The radiation efficiency of the spectral distribution by the illumination method according to the third embodiment of the present invention is preferably in the range of 180 (lm / W) to 320 (lm / W), and is a value of a normal incandescent bulb or the like. Was at least 20% higher than 150 (lm / W). This is presumably because radiation from the semiconductor light-emitting element and radiation from the phosphor are inherent, and there are appropriate irregularities at appropriate positions in the spectral distribution in relation to V (λ). From the viewpoint of compatibility with color appearance, the radiation efficiency of the illumination method of the present invention is preferably in the following range.

The radiation efficiency K by the illumination method according to the third embodiment of the present invention is preferably 180 (lm / W) or more, but is preferably 205 (lm / W) or more, preferably 208. (Lm / W) or higher, and very preferably 215 (lm / W) or higher. On the other hand, the radiation efficiency K is ideally high, but in the present invention, it is preferably 320 (lm / W) or less, and 282 (lm / W) or less from the balance with the color appearance. Is slightly preferred, preferably 232 (lm / W) or less, and particularly preferably 231 (lm / W) or less.
In addition, the examination using the actual test light was made in the visual experiment, and the preferable range of K inside the preferable experiment result under the examination was 206 (lm / W) or more and 288 (lm / W) or less. .

、
ΔＣ_ｎ、（ΔＣ_ｍａｘ−ΔＣ_ｍｉｎ）をより適切な値とするためには、本発明の照明方法において、ＣＣＴは４０００Ｋに近い値をとることが好ましかった。これは４０００Ｋ付近の光は基準の光を見てもその分光分布が波長にあまり依存せずに等エネルギー的であって、基準の光に対して容易に凹凸を形成した試験光分光分布が実現できるためと考えられる。換言すると、他のＣＣＴの場合と比較しても、｜Δｈ_ｎ｜と（ΔＣ_ｍａｘ−ΔＣ_ｍｉｎ）を比較的小さく保持したまま、

を増加させ、大多数の色票に対するΔＣ_ｎを所望の値に容易に制御可能である。 Furthermore, the following was found regarding CCT in the illumination method according to the third embodiment of the present invention. Various indexes determined to be preferable by comparative visual experiments, that is, | Δh _n |,

,
In order to set ΔC _n and (ΔC _max −ΔC _min ) to a more appropriate value, it is preferable that the CCT has a value close to 4000K in the illumination method of the present invention. This is because the spectral distribution of light around 4000K is isoenergetic regardless of the wavelength even if the reference light is viewed, and a test light spectral distribution in which irregularities are easily formed with respect to the reference light is realized. This is thought to be possible. In other words, | Δh _n | and (ΔC _max −ΔC _min ) are kept relatively small as compared with other CCT cases.

And ΔC _n for the majority of color charts can be easily controlled to a desired value.

Therefore, the CCT in the illumination method according to the third embodiment of the present invention is preferably slightly from 1800K to 15000K, preferably from 2000K to 10,000K, more preferably from 2300K to 7000K, and from 2600K to 6600K. It is very particularly preferred that it is 2900K to 5800K, and most preferred is 3400K to 5100K.
In addition, the examination using the actual test light was made in the visual experiment, and the preferable range of CCT inside the preferable experimental result under the examination was 2550 (K) or more and 5650 (K) or less.

、
ΔＣ_ｎ、（ΔＣ_ｍａｘ−ΔＣ_ｍｉｎ）を指標としてまとめた。なお、｜Δｈ_ｎ｜、ΔＣ_ｎは、ｎを
選択すると値が変化するが、ここでは最大値と最小値を示した。これらの値も表８に合わせて記載した。なお、第五ステップにおける検討は、本発明に係る実施例、比較例をも表すものである。 [Fifth step details Study on control elements]
In the fifth step, the control element is introduced into the LED light source / apparatus / system that does not include the control element, which is prototyped in the second step, and the radiometric characteristics of the spectral distribution of the light emitted by the light emitting device including the control element Attempts were made to extract the photometric characteristics from the measured spectrum. In other words, numerical features such as index A _cg , radiation efficiency K (lm / W), CCT (K), and D _{uv of} light emitted from the light emitting device in the main radiation direction were extracted. At the same time, the difference between the appearance of the color of the 15-color chart assumed when illuminated with the reference light for calculation and the appearance of the color of the 15-color chart assumed when illuminated with the measured test light spectral distribution is also used. , | Δh _n |,

,
ΔC _n and (ΔC _max −ΔC _min ) were collected as indices. The values of | Δh _n | and ΔC _n change when n is selected, but the maximum value and the minimum value are shown here. These values are also shown in Table 8. Note that the study in the fifth step also represents examples and comparative examples according to the present invention.

Next, by including the control element, how the total radiation spectral distribution Φ _elm (λ) of the light emitted by the light emitting element and the spectral distribution Φ _SSL (λ) of the light emitted in the main direction by the light emitting device change. I did some experiments.
Hereinafter, an experiment according to the present invention will be described.

As described in the light-emitting element column of Reference Example 1 in Table 8, a packaged LED including a purple LED as a semiconductor light-emitting element and SBCA, β-SiAlON, and CASON as light-emitting elements as a phosphor material was manufactured. The relative total radiant flux spectral distribution Φ _elmrel (λ) of all the light-emitting elements obtained by adjusting the radiant intensity of the purple LED and the radiant intensity from each phosphor and obtained in the wavelength range of 380 nm to 780 nm is shown by the dotted line in FIG. I made it. The relative total radiant flux spectral distribution Φ _elmrel (λ) is obtained by measuring the total radiant flux spectral distribution Φ _elm (λ) of the package LED in the wavelength region of 380 nm to 780 nm using an integrating sphere, and then obtained at a wavelength of 632 nm. It was obtained by dividing the total radiant flux spectral distribution Φ _elm (λ) by the maximum radiant flux spectral intensity Φ _elmmax obtained. The various radiometric, photometric and colorimetric characteristics obtained from Φ _elmrel (λ) were good as summarized in Reference Example 1 in Table 8.
Next, a package LED module was manufactured using three of the package LEDs having the same performance. Further, a light emitting device was manufactured using the packaged LED module and the Fresnel lens. The Fresnel lens base material is mixed with a light absorbing material for a specific wavelength so as to have an optical filter function. Next, light emitted from the light emitting device in the vertical direction, which is the main radiation direction, was received by an optical fiber, and the spectral distribution of the partial radiant flux of the light emitting device was measured. The solid line in FIG. 45 is the maximum partial radiant flux intensity of the light emitting device at 632 nm given the maximum total radiant flux spectral intensity of the package LED, and is a relative spectral distribution obtained by dividing the spectral distribution of the partial radiant flux of the light emitting device. .

As is apparent from FIG. 45, as an effect of the Fresnel lens having the light absorbing material, the emission in the violet region near 400 nm is relatively suppressed, and the radiation having a longer wavelength than in the vicinity of 700 nm is also relatively suppressed.
Furthermore, the indices described in the conditions 1 to 11 calculated from the relative total radiant flux spectral distribution from the package LED indicated by the dotted line in FIG. 45 and the relative spectral distribution of the partial radiant flux emitted on the axis from the light emitting device are: It was as Table 9. Various radiometric, photometric and colorimetric characteristics obtained from φ _SSL (λ) of the partial radiant flux emitted on the axis from the light emitting device are summarized in Example 1 in Table 8. It was as good as it was.

Furthermore, it is assumed that the relative total radiant flux spectral distribution from the packaged LED (without the control element) in FIG. 45 and the calculation reference light (black body radiation light) having the corresponding CCT are illuminated. FIG. 46 shows a CIELAB plot in which the a ^* value and b ^* value of the 15 types of modified Munsell color charts are plotted. In addition, when the relative spectral distribution radiated on the axis from the light emitting device (with control elements) in FIG. 45 and the calculation reference light (black body radiation light) having the corresponding CCT are respectively illuminated. FIG. 47 shows a CIELAB plot in which both the a ^* value and the b ^* value of the assumed 15 types of corrected Munsell color charts are plotted.

In the same manner as in Reference Example 1 and Example 1, experiments were also conducted on Reference Example 2 and Example 2. The results are shown in Tables 8 and 9 and FIGS.
In the same manner as in Reference Example 1 and Example 1, experiments were also conducted on Reference Example 3 and Example 3. The results are shown in Table 8, Table 9 and FIGS.
In the same manner as in Reference Example 1 and Example 1, experiments were also conducted on Reference Example 4 and Example 4. The results are shown in Tables 8 and 9 and FIGS.
In addition, as reference comparative example 1, when the driving voltage is adjusted and a commercially available incandescent bulb is set to 2700K, and as in comparative example 1, a commercially available neodymium bulb is used, the same as in example 1, radiometric and photometric The measurement and derivation were performed with respect to the parameters described in physics, colorimetric characteristics, and various conditions 1-11. The results are shown in Tables 8 and 9 and FIGS.
Here, in the neodymium bulb, neodymium is doped in the glass portion of the incandescent bulb, which functions as a light absorbing material, and the glass surface functions as an optical filter in the visible range.

From these results, when the light emitting device according to the first embodiment of the present invention satisfies the following conditions 1 to 3, a light emitting device that exhibits the effects of the present invention can be achieved. Moreover, it can be considered that it becomes a preferred embodiment of the present invention by satisfying any or all of the conditions 4 to 11.
<Condition 1>
First, in the light emitting device according to the first embodiment of the present invention, 0.70 ≦ φ _SSLrel (λ) / Φ _elmrel (λ) ≦ 1.30 is satisfied in all _{λs of} 530 nm ≦ λ ≦ 580 nm. is important. The maximum specific luminous efficiency in the bright field is obtained at 555 nm. However, the condition 1 is that the total radiant flux spectral distribution of the light emitting element by the control element is 530 nm to 580 nm, which is a green region in the vicinity of the 555 nm, which is an extremely high visibility. It means that the influence of the shape change on is small. In particular, the wavelength region in this range is a region where the visibility is very high, which means that there is little change that leads to a reduction in luminous efficiency. Therefore, when the light-emitting device of the present invention is used, it is possible to realize a light-emitting device that does not cause a significant decrease in efficiency, does not deteriorate an illumination object, and has good color appearance.
<Condition 4>
Condition 1 is that 0.90 ≦ φ _SSLr in all λ of 530 nm ≦ λ ≦ 580 nm.
It is preferable that _el (λ) / Φ _elmrel (λ) ≦ 1.10.

<Condition 2>
Next, in the light emitting device according to the first embodiment of the present invention, φ _SSLrel (λ) / Φ _elmrel (λ) ≦ 0.97 or 1.03 ≦ φ _SSLrel (λ) / at 380 nm ≦ λ ≦ 780 nm. It is important that λ that satisfies Φ _elmrel (λ) exists. Condition 2 means that in the visible light region of 380 nm ≦ λ ≦ 780 nm, there is a portion where the influence of the shape change on the total radiant flux spectral distribution of the light emitting element by the control element occurs at any wavelength. .
<Condition 3>
Further, in the light emitting device according to the first embodiment of the present invention, the distance D _UVSSL from the black body radiation locus defined by ANSI C78.377 related to φ _SSLrel (λ) is 380 nm ≦ λ ≦ 780 nm, It is important that −0.0350 ≦ D _uvSSL ≦ −0.0040. Condition 3 is a necessary requirement for achieving a natural and preferable color appearance and a preferable object appearance described in the fourth step.

<Condition 5>
In the light emitting device according to the first embodiment of the present invention, it is preferable that 0.80 ≦ φ _SSLrel (λ) / Φ _elmrel (λ) ≦ 1.20 holds for all λ of 495 nm ≦ λ ≦ 590 nm. . Condition 5 has little influence of the shape change on the total radiant flux spectral distribution of the light emitting element by the control element in the outer area including the green area in the vicinity of 555 nm where the visibility is very high as shown in condition 1 Means that. In particular, the wavelength region in this range is a region where the visibility is relatively high, which means that there is little change that leads to a reduction in luminous efficiency. Therefore, when the light-emitting device of the present invention is used, it is possible to realize a light-emitting device that does not cause a significant decrease in efficiency, does not deteriorate an illumination object, and has good color appearance.

<Condition 6>
In the light emitting device according to the first embodiment of the present invention, φ _SSLrel (λ) / Φ _elmrel (λ) ≦ 0.70 or 1.30 ≦ φ _SSLrel (λ) / Φ _elmrel (at 380 nm ≦ λ ≦ 495 nm). It is preferable that λ satisfying λ) exists.
<Condition 7>
The light-emitting device according to the first embodiment of the present invention has a φ _{S of} 380 nm ≦ λ ≦ 495 nm.
It is preferable that λ satisfying _SLrel (λ) / Φ _elmrel (λ) ≦ 0.40 or 1.60 ≦ φ _SSLrel (λ) / Φ _elmrel (λ) exists.
<Condition 8>
In the light emitting device according to the first embodiment of the present invention, φ _SSLrel (λ) / Φ _elmrel (λ) ≦ 0.10 or 1.90 ≦ φ _SSLrel (λ) / Φ _elmrel (at 380 nm ≦ λ ≦ 495 nm). It is preferable that λ satisfying λ) exists.
Conditions 6 to 8 mean that the influence of the shape change on the total radiant flux spectral distribution of the light emitting element by the control element is large in the short wavelength region where the energy is relatively large in the visible region. In particular, the condition 6-8 means that the spectral radiant flux reduction of the light emitting element by the control element functions appropriately in the short wavelength region where the energy is relatively large in the visible region, and the deterioration of the illumination object is performed. Can be suppressed.

<Condition 9>
In the light emitting device according to the first embodiment of the present invention, φ _SSLrel (λ) / Φ _elmrel (λ) ≦ 0.70 or 1.30 ≦ φ _SSLrel (λ) / Φ _elmrel (at 590 nm ≦ λ ≦ 780 nm). It is preferable that λ satisfying λ) exists.
<Condition 10>
The light-emitting device according to the first embodiment of the present invention has φ _SSLrel (λ) / Φ _elmrel (λ) ≦ 0.40 or 1.60 ≦ φ _SSLrel (λ) / Φ _elmrel (590 nm ≦ λ ≦ 780 nm). It is preferable that λ satisfying λ) exists.
<Condition 11>
The light-emitting device according to the first embodiment of the present invention has φ _SSLrel (λ) / Φ _elmrel (λ) ≦ 0.10 or 1.90 ≦ φ _SSLrel (λ) / Φ _elmrel (590 nm ≦ λ ≦ 780 nm). It is preferable that λ satisfying λ) exists.
Conditions 9 to 11 mean that the influence of the shape change on the total radiant flux spectral distribution of the light emitting element by the control element is large in the long wavelength region that can be relatively heat in the visible region. In particular, the condition 9-11 means that the spectral radiant flux reduction of the light emitting element by the control element functions appropriately in the long wavelength region that can be relatively heat in the visible region, and the heat to the illumination target object Damage caused by can be suppressed.

Moreover, the aspect which satisfy | fills the following conditions 12-14 is also preferable for the light-emitting device which concerns on the 1st embodiment of this invention.
<Condition 12>
At 780 nm ≦ λ ≦ ₁₀₀₀₀ nm, there exists λ satisfying φ _SSLrel (λ) / Φ _elmrel (λ) ≦ 0.70 or 1.30 ≦ φ _SSLrel (λ) / Φ _elmrel (λ).
<Condition 13>
At 780 nm ≦ λ ≦ 10000 nm,
There _exists λ _satisfying φ _SSLrel (λ) / Φ _elmrel (λ) ≦ 0.40 or 1.60 ≦ φ _SSLrel (λ) / Φ _elmrel (λ).
<Condition 14>
At 780 nm ≦ λ ≦ 10000 nm,
There _exists λ _satisfying φ _SSLrel (λ) / Φ _elmrel (λ) ≦ 0.10 or 1.90 ≦ φ _SSLrel (λ) / Φ _elmrel (λ).
Conditions 12 to 14 mean that the influence of the shape change on the total radiant flux spectral distribution of the light emitting element by the control element is large in the infrared wavelength region including heat rays. In particular, the condition 12-14 means that the spectral radiant flux reduction of the light emitting element by the control element functions appropriately in the infrared wavelength region, and damage to the illumination object due to heat can be suppressed.

Preferred embodiments for carrying out the light-emitting device and illumination method of the present invention will be described below, but the mode for carrying out the light-emitting device and illumination method of the present invention is not limited to those used in the following description.

  The light-emitting device of the present invention emits light from the light-emitting device in the main radiation direction, and the light-measuring device is suitable if the radiometric characteristics and the photometric characteristics of the test light that is a color stimulus for the illumination object are within an appropriate range. There are no restrictions on the configuration, materials, etc.

  In the illumination method of the present invention, the fifteen colors are assumed assuming that the photometric characteristics of the test light that is emitted to the object to be illuminated and is a color stimulus are in an appropriate range and are illuminated with the reference light for calculation. If the difference between the color appearance of the vote and the color appearance of the 15-color chart assuming the illumination with the measured test light spectral distribution is within an appropriate range, there are no restrictions on the configuration, material, and the like of the light emitting device.

  A light emitting device such as an illumination light source for implementing the light emitting device or the illumination method of the present invention, a luminaire including the illumination light source, and a lighting system including the illumination light source or the luminaire includes at least a light emitting element and at least a control element. It is out. The light emitting element preferably includes a semiconductor light emitting element. The illumination light source including the semiconductor light emitting element may include, for example, a plurality of semiconductor light emitting elements of different types of blue, green, and red in one illumination light source. Including a light emitting element, including a green semiconductor light emitting element in a different illumination light source, and further including a red semiconductor light emitting element in a different illumination light source, these being a filter, lens, reflector, drive The lighting system may be integrated with a circuit or the like. Furthermore, there is one illumination light source in one luminaire, and a single semiconductor light emitting element is contained therein, and the illuminating method of the present invention or Although the light emitting device cannot be implemented, the light emitted as the lighting system may satisfy the desired characteristics at the position of the lighting object by additive color mixing with light from different lighting fixtures existing in the lighting system. Of course, the light in the main radiation direction among the light emitted as the illumination system may satisfy the desired characteristics. In any form, the light in the main radiation direction among the light emitted from the light emitting device or the light as the color stimulus that is finally irradiated to the illumination object is suitable for the present invention. It only has to satisfy the conditions.

  In the following, the light-emitting device according to the first embodiment of the present invention and the light-emitting device for carrying out the illumination method according to the third embodiment of the present invention are preferably satisfied after satisfying the appropriate conditions. Describe the properties that should be present.

  The light emitting device according to the first embodiment of the present invention or the light emitting device for carrying out the illumination method according to the third embodiment of the present invention is within a short wavelength region of Λ1 (380 nm) to Λ2 (495 nm). And another light emitting element (luminescent material) having a peak in the intermediate wavelength region of Λ2 (495 nm) to Λ3 (590 nm), and Λ3 ( It is preferable to have another light emitting element (light emitting material) having a peak in a long wavelength region from 590 nm to 780 nm. This is because it is possible to easily realize a preferable color appearance by independently setting or controlling the intensity of each light emitting element.

Therefore, the light-emitting device according to the first embodiment of the present invention or the light-emitting device for carrying out the illumination method according to the third embodiment of the present invention has a light emission peak in each of the above three wavelength regions. It is preferable to have at least one type of light-emitting element (light-emitting material), one type in two of the three wavelength regions, and the other one region to have a plurality of light-emitting elements (light-emitting materials). More preferably, it is very preferable that one of the three wavelength regions has one kind and the other two regions have a plurality of light emitting elements (light emitting materials). It is particularly preferred to have a light emitting element. This is because the control of the spectral distribution is remarkably improved by incorporating the light-emitting elements so as to have two or more peak wavelengths in one region, and mathematically, the color appearance of the illuminated object is desired. This is because it becomes easier to control.

  Therefore, in an actual light-emitting device using a semiconductor light-emitting element as an excitation light source for a phosphor, there are two types of phosphors in one light-emitting device, and the peak wavelength is set in each of the three wavelength regions together with the wavelength of the semiconductor light-emitting element. It is preferable to have. Furthermore, it is more preferable that there are three types of phosphors, and two types of light emitting elements are present in at least one of the three wavelength regions together with the wavelength of the semiconductor light emitting element. From such an idea, 4 or more types of phosphors are very preferable, and 5 types are extremely preferable. In particular, when six or more kinds of phosphors are present in one light source, the controllability of the spectrum is adversely reduced due to mutual absorption between the phosphors. In addition, from the viewpoint of realizing a simple light-emitting device from another viewpoint, the phosphor type may be one, and the light-emitting device may be configured with two types of light-emitting elements together with the light emission peak of the semiconductor light-emitting element. I do not care.

  The same applies to a case where an actual light-emitting device is configured by only semiconductor light-emitting elements having different peak wavelengths. That is, from the viewpoint of realizing a preferable spectral distribution, the number of semiconductor light emitting elements in one light source is preferably 3 or more, more preferably 4 or more, very preferably 5 or more, and 6 is particularly preferable. In the case of seven types or more, the complexity of mounting in the light source occurs, which is not preferable. In addition, from the viewpoint of realizing a simple light-emitting device different from this, the light-emitting device may be configured with two types of semiconductor light-emitting elements.

  It is also possible to freely mix and mount the semiconductor light emitting element and the phosphor, and the blue light emitting element and two kinds of phosphors (green and red) may be mounted in one light source. The element and three types of phosphors (green, red 1, red 2) may be mounted in one light source. Furthermore, you may mount a purple light emitting element and four types of fluorescent substance (blue, green, red 1, red 2) in 1 light source. Furthermore, a single light source is equipped with a blue light emitting element and two types of phosphors (green and red), and a purple light emitting element and three types of phosphors (blue, green and red). The portion that is present may be included.

  From the viewpoint of controlling the intensity of the peak portion and the intensity of the valley between the peaks, that is, from the viewpoint of forming appropriate unevenness in the spectral distribution, at least one of the light emitting elements (light emitting materials) in each of the three wavelength regions is relatively It preferably includes a narrow band light emitting element. Conversely, it is difficult to form appropriate irregularities in the spectral distribution only with a light emitting element having a width comparable to the width of each of the three wavelength regions. Therefore, in the present invention, it is preferable that at least one includes a light emitting element having a relatively narrow band, but further includes light emitting elements having a relatively narrow band in two of the three wavelength regions. More preferably, it includes a relatively narrow-band light-emitting element in all three wavelength regions. In this case, the light emitting element having a relatively narrow band may be a light emitting element in a wavelength region where only the light emitting element is present, but there are a plurality of types of light emitting elements having a relatively narrow band in the wavelength region. It is more preferable that the light emitting element having a relatively narrow band and the light emitting element having a relatively wide band are both present in the wavelength region.

In addition, the comparatively narrow band here means that the full width at half maximum of the light emitting element (light emitting material) is a short wavelength region (380 nm to 495 nm), an intermediate wavelength region (495 nm to 590 nm), and a long wavelength region (590 nm to 780 nm). That is, 2/3 or less with respect to the respective region widths of 115 nm, 95 nm and 190 nm. Further, among the light emitting elements having a relatively narrow band, the full width at half maximum is preferably 1/2 or less, more preferably 1/3 or less, and 1/4 or less with respect to the width of each region. It is very preferable that it is 1/5 or less. In addition, an excessively narrow narrow band spectrum may not achieve a desired characteristic unless a plurality of types of light emitting elements are mounted in the light emitting device. Therefore, the full width at half maximum is preferably 2 nm or more, and 4 nm or more. More preferably, 6 nm or more is very preferable, and 8 nm or more is particularly preferable.

、
ΔＣ_ｎ、（ΔＣ_ｍａｘ−ΔＣ_ｍｉｎ）等を適切な数値範囲にしやすくなるために好ましい。さらに、比較的狭帯域の蛍光体を用いると、広帯域蛍光体を用いる場合よりもＤ_ｕｖ制御も容易になるために好ましい。 From the viewpoint of realizing a desired spectral distribution, when a combination of light emitting elements (light emitting materials) having a relatively narrow band is used, it is easy to form an uneven shape in the spectral distribution, and an appropriate range is clear through visual experiments. The index A _cg , the radiation efficiency K (lm / W), and the like are preferable because they are easily set to desired values. Also, the difference between the color appearance of the 15 color chart when the light is regarded as a color stimulus and the illumination with the light emitting device is assumed and the color appearance when the illumination with the calculation reference light is assumed By incorporating a relatively narrow band in the light emitting element, a suitable range has been revealed by saturation control, particularly visual experiments | Δh _n |,

,
It is preferable because ΔC _n , (ΔC _max −ΔC _min ), etc. can be easily set to an appropriate numerical range. Furthermore, it is preferable to use a relatively narrow-band phosphor because the D _uv control becomes easier than in the case of using a broadband phosphor.

  Further, in the light emitting device of the present invention, a part of the spectral distribution is absorbed, reflected, condensed, etc. by the control element with respect to the broadband total radiant flux spectral distribution emitted from the light emitting element. A narrow-band spectral distribution can also be realized, which is preferable.

  In the light emitting device and the illumination method of the present invention, it is preferable that the following light emitting material, phosphor material, and semiconductor light emitting element are inherent in the light emitting device as a light emitting element.

  First, in the short wavelength region of Λ1 (380 nm) to Λ2 (495 nm) in the three wavelength regions, heat radiation from a hot filament, discharge radiation from a fluorescent tube, high pressure sodium lamp, etc., laser, etc. It is possible to include light emitted from any light source such as spontaneous emission light, spontaneous emission light from a semiconductor light emitting element, spontaneous emission light from a phosphor, and the like. Among these, light emission from a photoexcited phosphor, light emission from a semiconductor light emitting element, and light emission from a semiconductor laser are preferable because they are small in size, high in energy efficiency, and capable of relatively narrow band light emission.

Specifically, the following is preferable.
As a semiconductor light emitting element, a purple light emitting element (peak wavelength is about 395 nm to about 420 nm) including a In (Al) GaN-based material formed on a sapphire substrate or a GaN substrate in an active layer structure, a blue purple light emitting element (peak A blue light emitting element (having a peak wavelength of about 455 nm to 485 nm) is preferable. Further, a blue light emitting element (peak wavelength is about 455 nm to 485 nm) containing Zn (Cd) (S) Se-based material formed on a GaAs substrate in the active layer structure is also preferable.

Note that the spectral distribution of the radiant flux exhibited by light emitting elements (light emitting materials) such as semiconductor light emitting elements and phosphors, and the peak wavelength thereof are the ambient temperature, the heat radiation environment of light emitting devices such as packages and lamps, injection current, circuit configuration, Or, in some cases, it is usually slightly changed due to deterioration or the like. Therefore, a semiconductor light emitting device having a peak wavelength of 418 nm under a certain driving condition may exhibit a peak wavelength of 421 nm, for example, when the temperature of the surrounding environment increases.
The same applies to the spectral distribution of the radiant flux and the peak wavelength exhibited by light emitting elements (light emitting materials) such as semiconductor light emitting elements and phosphors described below.

  The active layer structure may be a multiple quantum well structure in which a quantum well layer and a barrier layer are stacked, or a single or double hetero structure including a relatively thick active layer and a barrier layer (or a clad layer), which consists of a single pn junction. It may be homozygous.

In particular, when the active layer contains an In (Al) GaN-based material, the blue-violet light-emitting element and the violet light-emitting element whose In concentration is lower in the active layer structure than the blue light-emitting element are emitted by the segregation of In. This is preferable because fluctuation is reduced and the full width at half maximum of the emission spectrum is reduced. Further, the blue-violet light-emitting element and the violet light-emitting element are preferable because they are positioned relatively on the outer side (short wavelength side) of wavelengths from 380 nm to 495 nm, which is the wavelength region, and D _uv can be easily controlled. That is, in the present invention, the semiconductor light emitting device having a light emission peak in the short wavelength region of Λ1 (380 nm) to Λ2 (495 nm) is preferably a blue light emitting device (peak wavelength is about 455 nm to 485 nm), and a blue-violet color having a shorter wavelength than this. A light emitting element (peak wavelength is about 420 nm to about 455 nm) is more preferable, and a purple light emitting element (peak wavelength is about 395 nm to about 420 nm) is very preferable. It is also preferable to use a plurality of these light emitting elements.

  It is also preferable to use a semiconductor laser as the light emitting element. For the same reason as described above, a blue semiconductor laser (oscillation wavelength is about 455 nm to 485 nm) is preferable, and a blue-violet semiconductor laser having a longer wavelength (oscillation wavelength from 420 nm) is preferable. About 455 nm) is more preferable, and a violet semiconductor laser (with an oscillation wavelength of about 395 nm to 420 nm) is very preferable.

  The semiconductor light emitting element in the short wavelength region used in the light emitting device or illumination method of the present invention preferably has a narrow full width at half maximum of its emission spectrum. In this respect, the full width at half maximum of the semiconductor light emitting element used in the short wavelength region is preferably 45 nm or less, more preferably 40 nm or less, very preferably 35 nm or less, and particularly preferably 30 nm or less. In addition, since an extremely narrow band spectrum may not be able to realize desired characteristics unless many types of light emitting elements are mounted in the light emitting device, the full width at half maximum of the semiconductor light emitting element used in the short wavelength region is 2 nm or more. Is preferable, 4 nm or more is more preferable, 6 nm or more is very preferable, and 8 nm or more is particularly preferable.

  The semiconductor light-emitting element in the short wavelength region used in the light-emitting device or illumination method of the present invention preferably includes an In (Al) GaN-based material in the active layer structure, and thus is formed on a sapphire substrate or a GaN substrate. A light emitting element is preferable. In particular, the degree of In segregation in the active layer of the light emitting device formed on the GaN substrate is better than that formed on the sapphire substrate. This depends on the lattice matching between the substrate and the active layer structure material. For this reason, since the full width at half maximum of the In (Al) GaN emission spectrum on the GaN substrate can be made narrower, a remarkable synergistic effect with the present invention can be expected, which is very preferable. Furthermore, even if it is a light emitting element on a GaN substrate, the element formed especially on the semipolar surface and the nonpolar surface is preferable. This reduces the piezoelectric polarization effect with respect to the crystal growth direction, which increases the spatial overlap of the spatial electron and hole wave functions in the quantum well layer, which in principle improves luminous efficiency and narrows the spectrum. This is because bandwidth can be realized. Therefore, it is very preferable to use a semiconductor light emitting element on a semipolar or nonpolar GaN substrate because a remarkable synergistic effect with the present invention can be expected.

  Further, it is preferable that the thickness of the substrate is either thick or completely separated from the semiconductor light emitting element. In particular, when a semiconductor light emitting device having a short wavelength region is formed on a GaN substrate, the substrate is preferably thick, preferably 100 μm or more, more preferably 200 μm or more, so as to facilitate light extraction from the side wall of the GaN substrate. 400 μm or more is very preferable, and 600 μm or more is particularly preferable. On the other hand, the thickness of the substrate is preferably 2 mm or less, more preferably 1.8 mm or less, very preferably 1.6 mm or less, and particularly preferably 1.4 mm or less from the viewpoint of device preparation.

  On the other hand, when a light emitting element is formed on a sapphire substrate or the like, the substrate is preferably peeled off by a method such as laser lift-off. In this way, the stress applied to the quantum well layer that promotes the broadband due to the extreme lattice mismatch with the substrate is reduced, and as a result, the spectrum of the light emitting element can be narrowed. Therefore, a light-emitting element from which a sapphire substrate or the like is peeled off can be expected to have a remarkable synergistic effect with the present invention, which is very preferable.

  It is preferable that the full width at half maximum of the phosphor material in the short wavelength region used in the light emitting device or the illumination method of the present invention is narrow. From this viewpoint, the full width at half maximum of the emission spectrum of the phosphor material used in the short wavelength region when excited at room temperature is preferably 90 nm or less, more preferably 80 nm or less, very preferably 70 nm or less, and particularly 60 nm or less. Is preferable. In addition, since an extremely narrow band spectrum may not be able to realize desired characteristics unless a plurality of types of light emitting elements are mounted in the light emitting device, the full width at half maximum of the phosphor material used in the short wavelength region is 2 nm or more. Is preferable, 4 nm or more is more preferable, 6 nm or more is very preferable, and 8 nm or more is particularly preferable.

The phosphor material in the short wavelength region preferably has a peak wavelength in the following range in consideration of the convenience of exciting the phosphor material and the controllability of D _uv . In the case of photoexcitation, the peak wavelength is preferably from 455 nm to 485 nm, and more preferably from 420 nm to 455 nm, which has a shorter wavelength. On the other hand, in the case of electron beam excitation, the peak wavelength is preferably from 455 nm to 485 nm, more preferably from 420 nm to 455 nm, which is shorter than this, and the peak wavelength is very preferably from 395 nm to 420 nm. .

As a specific example of the phosphor material in the short wavelength region used in the light emitting device or the illumination method of the present invention, any phosphor material satisfying the full width at half maximum can be preferably used, but alkaline earth aluminin using Eu ²⁺ as an activator. There are blue phosphors based on crystals of acid salts or alkaline earth halophosphates. More specifically, a phosphor represented by the following general formula (5), a phosphor represented by the following general formula (5) ′, (Sr, Ba) ₃ MgSi ₂ O ₈ : Eu ²⁺ , and (Ba, Sr, Ca, Mg) Si ₂ O ₂ N ₂ : Eu.
(Ba, Sr, Ca) MgAl ₁₀ O ₁₇ : Mn, Eu (5)
(The alkaline earth aluminate phosphor represented by the general formula (5) is referred to as a BAM phosphor.)
_{Sr a Ba b Eu x (PO} 4) c X d (5) '
(In the general formula (5) ′, X is Cl. Also, c, d and x are 2.7 ≦ c ≦ 3.3, 0.9 ≦ d ≦ 1.1, 0.3 ≦ x ≦. In addition, a and b satisfy the conditions of a + b = 5-x and 0 ≦ b / (a + b) ≦ 0.6) (general formula (5)
Among the alkaline earth halophosphate phosphors represented by ′, those containing Ba are called SBCA phosphors, and those containing no Ba are called SCA phosphors. )
These phosphors, BAM phosphor, SBCA phosphor, SCA phosphor, and Ba-SION phosphor ((Ba, Sr, Ca, Mg) Si ₂ O ₂ N ₂ : Eu), (Sr, Ba) Preferred examples include ₃ MgSi ₂ O ₈ : Eu ²⁺ phosphor.

  Next, in the intermediate wavelength region from Λ2 (495 nm) to Λ3 (590 nm) in the three wavelength regions, thermal radiation from a hot filament, discharge radiation from a fluorescent tube, high-pressure sodium lamp, etc., nonlinear optical effect It is possible to include light emitted from any light source such as stimulated emission light from a laser including second harmonic generation (SHG) using SEM, spontaneous emission light from a semiconductor light emitting device, spontaneous emission light from a phosphor, etc. is there. Among these, light emission from a photoexcited phosphor, light emission from a semiconductor light emitting element, light emission from a semiconductor laser, and an SHG laser are preferable because they are small in size, high in energy efficiency, and capable of relatively narrow band light emission. .

Specifically, the following is preferable.
As a semiconductor light emitting device, a blue-green light emitting device (peak wavelength is about 495 nm to about 500 nm) or a green light emitting device (peak wavelength is 500 nm) containing an In (Al) GaN-based material on a sapphire substrate or a GaN substrate in an active layer structure. To 530 nm), a yellow-green light emitting element (peak wavelength is about 530 nm to 570 nm), and a yellow light emitting element (peak wavelength is about 570 nm to 580 nm). Further, a yellow-green light emitting element by GaP on the GaP substrate (peak wavelength is about 530 nm to 570 nm) and a yellow light emitting element by GaAsP on the GaP substrate (peak wavelength is about 570 nm to 580 nm) are also preferable. Furthermore, a yellow light emitting element (peak wavelength is about 570 nm to about 580 nm) by AlInGaP on a GaAs substrate is also preferable.

The active layer structure may be a multiple quantum well structure in which a quantum well layer and a barrier layer are stacked, or a single or double hetero structure including a relatively thick active layer and a barrier layer (or a clad layer), which consists of a single pn junction. It may be homozygous.
In particular, when an In (Al) GaN-based material is used, the yellow-green light-emitting element, the green light-emitting element, and the blue-green light-emitting element whose In concentration is lower in the active layer structure than the yellow light-emitting element Is preferable because the fluctuation of the emission wavelength due to is reduced and the full width at half maximum of the emission spectrum is reduced. That is, in the present invention, the semiconductor light emitting device having a light emission peak in the intermediate wavelength region of Λ2 (495 nm) to Λ3 (590 nm) is preferably a yellow light emitting device (peak wavelength is about 570 nm to 580 nm), and a yellowish green having a shorter wavelength than this. A light emitting element (peak wavelength is about 530 nm to 570 nm) is more preferable, a green light emitting element having a shorter wavelength (peak wavelength is about 500 nm to about 530 nm) is very preferable, and a blue-green light emitting element (peak wavelength is about 495 nm to about 500 nm). It is particularly preferable.

It is also preferable to use a semiconductor laser, a SHG laser in which the oscillation wavelength of the semiconductor laser is wavelength-converted by a nonlinear optical effect, or the like as the light emitting element. The oscillation wavelength is preferably in the yellow (peak wavelength is about 570 nm to 580 nm) region for the same reason as described above, and in the yellow-green region (the peak wavelength is about 530 nm to 570 nm) shorter than this. More preferably, it is very preferable to be in the green region (peak wavelength is about 500 nm to 530 nm) with a shorter wavelength than this, and it is particularly preferable to be in the blue green region (peak wavelength is about 495 nm to 500 nm). Is preferred.
The semiconductor light emitting element in the intermediate wavelength region used in the illumination method or the light emitting device of the present invention preferably has a narrow full width at half maximum of its emission spectrum. From this viewpoint, the full width at half maximum of the semiconductor light emitting element used in the intermediate wavelength region is preferably 75 nm or less, more preferably 60 nm or less, very preferably 50 nm or less, and particularly preferably 40 nm or less. In addition, since an extremely narrow band spectrum may not be able to realize desired characteristics unless many types of light emitting elements are mounted in the light emitting device, the full width at half maximum of the semiconductor light emitting element used in the intermediate wavelength region is 2 nm or more. Is preferable, 4 nm or more is more preferable, 6 nm or more is very preferable, and 8 nm or more is particularly preferable.

The semiconductor light emitting device in the intermediate wavelength region used in the present invention is preferably a light emitting device formed on a sapphire substrate or a GaN substrate when an In (Al) GaN-based material is included in the active layer structure. In particular, a light emitting element formed on a GaN substrate is more preferable. In order to create an InAlGaN-based device in the intermediate wavelength region, it is necessary to introduce a relatively large amount of In into the active layer structure, but when it is formed on a GaN substrate, it is formed on a sapphire substrate. This is because the piezoelectric effect due to the difference in lattice constant from the substrate is reduced compared to the case, and the spatial separation of electrons / holes when carriers are injected into the quantum well layer can be suppressed. As a result, the full width at half maximum of the emission wavelength can be narrowed. Therefore, in the present invention, a light emitting element in the intermediate wavelength region on the GaN substrate is preferable because a remarkable synergistic effect is expected. Furthermore, even if it is a light emitting element on a GaN substrate, the element formed especially on the semipolar surface and the nonpolar surface is preferable. This reduces the piezoelectric polarization effect with respect to the crystal growth direction, which increases the spatial overlap of the spatial electron and hole wave functions in the quantum well layer, which in principle improves luminous efficiency and narrows the spectrum. This is because bandwidth can be realized. Therefore, it is very preferable to use a semiconductor light emitting element on a semipolar or nonpolar GaN substrate because a remarkable synergistic effect with the present invention can be expected.

Regardless of the semiconductor light emitting element formed on any substrate, it is preferable that the thickness of the substrate is either thick or completely removed.
In particular, when a semiconductor light emitting device having an intermediate wavelength region is formed on a GaN substrate, the substrate is preferably thick, preferably 100 μm or more, more preferably 200 μm or more, so as to facilitate light extraction from the side wall of the GaN substrate. 400 μm or more is very preferable, and 600 μm or more is particularly preferable. On the other hand, the thickness of the substrate is preferably 2 mm or less, more preferably 1.8 mm or less, very preferably 1.6 mm or less, and particularly preferably 1.4 mm or less from the viewpoint of device preparation.

  Similarly, when a semiconductor light emitting device having an intermediate wavelength region is formed on a GaP substrate, the substrate is preferably thick, preferably 100 μm or more, and 200 μm or more so as to promote light extraction from the GaP substrate side wall. More preferably, 400 μm or more is very preferable, and 600 μm or more is particularly preferable. On the other hand, the thickness of the substrate is preferably 2 mm or less, more preferably 1.8 mm or less, very preferably 1.6 mm or less, and particularly preferably 1.4 mm or less from the viewpoint of device preparation.

  On the other hand, in the case of an AlInGaP-based material formed on a GaAs substrate, the band gap of the substrate is smaller than the band gap of the material forming the active layer structure, so that light in the emission wavelength region is absorbed. For this reason, the case where the thickness of a board | substrate is thin is preferable, and the case where it peeled completely from the semiconductor light-emitting device is preferable.

  Furthermore, when a semiconductor light emitting element is formed on a sapphire substrate or the like, it is preferable to peel off the substrate by a method such as laser lift-off. In this way, the stress applied to the quantum well layer, which is broadened due to an extreme lattice mismatch with the substrate, is reduced, and as a result, the spectrum of the light emitting element can be narrowed. Therefore, a semiconductor light emitting device from which a sapphire substrate or the like is peeled off can be expected to have a significant synergistic effect with the present invention, and is very preferable.

It is preferable that the full width at half maximum of the phosphor material in the intermediate wavelength region used in the light emitting device or the illumination method of the present invention is narrow. In this respect, the full width at half maximum of the emission spectrum of the phosphor material used in the intermediate wavelength region when excited at room temperature is preferably 130 nm or less, more preferably 110 nm or less, very preferably 90 nm or less, and particularly 70 nm or less. Is preferred. In addition, since an extremely narrow band spectrum may not be able to realize desired characteristics unless many types of light emitting elements are mounted in the light emitting device, the full width at half maximum of the phosphor material used in the intermediate wavelength region is 2 nm or more. Is preferable, 4 nm or more is more preferable, 6 nm or more is very preferable, and 8 nm or more is particularly preferable.
In the phosphor material in the intermediate wavelength region, the peak wavelength is 495 in consideration of D _uv controllability.
The case where the peak wavelength is from 500 nm to 530 nm and the case where the peak wavelength is from 570 nm to 580 nm are more preferable, and the peak wavelength is very preferably from 530 nm to 570 nm.

As a specific example of the phosphor material in the intermediate wavelength region used in the light emitting device or the illumination method of the present invention, any phosphor material satisfying the full width at half maximum can be preferably used. Specific examples thereof include green phosphors containing Eu ²⁺ , Ce ^3+, etc. as activators. A suitable green phosphor using Eu ²⁺ as an activator is a green phosphor based on a crystal composed of alkaline earth silicate, alkaline earth silicate nitride or sialon. This type of green phosphor can usually be excited using ultraviolet to blue semiconductor light emitting devices.

Specific examples of an alkaline earth silicate crystal as a base include a phosphor represented by the following general formula (6) and a phosphor represented by the following general formula (6) ′. _{(Ba a Ca b Sr c Mg} d Eu x) SiO 4 (6)
(In the general formula (6), a, b, c, d and x are a + b + c + d + x = 2, 1.0 ≦ a ≦ 2.0, 0 ≦ b <0.2, 0.2 ≦ c ≦ 0.8, 0 ≦ d <0.2
And 0 <x ≦ 0.5. (The alkaline earth silicate represented by the general formula (6) is called a BSS phosphor.)
Ba _1-xy Sr _x Eu _y Mg _1-z Mn _z Al ₁₀ O ₁₇ (6) ′
(In the general formula (6) ′, x, y, and z satisfy 0.1 ≦ x ≦ 0.4, 0.25 ≦ y ≦ 0.6, and 0.05 ≦ z ≦ 0.5, respectively.) (The alkaline earth aluminate phosphor represented by the formula (6) ′ is referred to as a G-BAM phosphor.)

Specific examples of the sialon crystal as a base include a phosphor represented by Si _6-z Al _z O _z N _8-z : Eu (where 0 <z <4.2) (this is expressed as β- Called SiAlON phosphor). Suitable green phosphors using Ce ³⁺ as an activator include green phosphors based on garnet-type oxide crystals, such as Ca ₃ (Sc, Mg) ₂ Si ₃ O ₁₂ : Ce and alkaline earths There are green phosphors based on metal scandate crystals, such as CaSc ₂ O ₄ : Ce. Other examples include SrGaS ₄ : Eu ²⁺ .
Still another example is an oxynitride phosphor represented by (Ba, Ca, Sr, Mg, Zn, Eu) ₃ Si ₆ O ₁₂ N ₂ (this is referred to as a BSON phosphor).

_{Others, (Y 1-u Gd u} ) 3 (Al 1-v Ga v) 5 O 12: Ce, Eu ( wherein each u and v are 0 ≦ u ≦ 0.3, and 0 ≦ v ≦ 0.5 Yttrium / aluminum / garnet phosphor (referred to as YAG phosphor). Ca _1.5x La _3−X Si ₆ N ₁₁ : Ce (where x is 0 ≦ x ≦ 1) and a lanthanum silicon nitride phosphor (referred to as an LSN phosphor).

Among these phosphors, BSS phosphors, β-SiAlON phosphors, BSON phosphors, G-BAM phosphors, YAG phosphors, SrGaS ₄ : Eu ²⁺ phosphors and the like can be preferably exemplified.

  Next, in the long wavelength region from Λ3 (590 nm) to 780 nm among the three wavelength regions, stimulated emission from thermal radiation from a hot filament, discharge radiation from a fluorescent tube, high-pressure sodium lamp, etc., laser, etc. Light emitted from any light source such as light, spontaneous emission from a semiconductor light emitting device, spontaneous emission from a phosphor, and the like can be included. Among these, light emission from a photoexcited phosphor, light emission from a semiconductor light emitting element, and light emission from a semiconductor laser are preferable because they are small in size, high in energy efficiency, and capable of relatively narrow band light emission.

Specifically, the following is preferable.
As the semiconductor light emitting element, an AlGaAs material formed on a GaAs substrate, an orange light emitting element including an (Al) InGaP material formed on a GaAs substrate in an active layer structure (peak wavelength is about 590 nm to about 600 nm), Red light emitting elements (600 nm to 780 nm) are preferred. A red light emitting element (600 nm to 780 nm) including a GaAsP-based material formed on a GaP substrate in the active layer structure is preferable.

  The active layer structure may be a multiple quantum well structure in which a quantum well layer and a barrier layer are stacked, or a single or double hetero structure including a relatively thick active layer and a barrier layer (or a clad layer), which consists of a single pn junction. It may be homozygous.

In particular, in this wavelength region, the peak wavelength is preferably close to 630 nm in consideration of both D _uv controllability and radiation efficiency. In this respect, the red light emitting element is more preferable than the orange light emitting element. That is, in the present invention, the semiconductor light emitting device having an emission peak in the long wavelength region from Λ3 (590 nm) to 780 nm is preferably an orange light emitting device (peak wavelength is about 590 nm to 600 nm), and a red light emitting device (peak wavelength is 600 nm to 780 nm). A red light emitting element having a peak wavelength close to about 630 nm is very preferable. In particular, a red light emitting device having a peak wavelength of 615 nm to 645 nm is very preferable.

  It is also preferable to use a semiconductor laser as the light emitting element. For the same reason as described above, the oscillation wavelength preferably has an oscillation wavelength in an orange (peak wavelength is about 590 to 600 nm) region, and has an oscillation wavelength in a red (peak wavelength about 600 to 780 nm) region. More preferably, the oscillation wavelength is very preferably in the red region close to about 630 nm. In particular, a red semiconductor laser having an oscillation wavelength of 615 nm to 645 nm is very preferable.

  The long-wavelength region semiconductor light-emitting element used in the light-emitting device or illumination method of the present invention preferably has a narrow full width at half maximum of its emission spectrum. In this respect, the full width at half maximum of the semiconductor light emitting element used in the long wavelength region is preferably 30 nm or less, more preferably 25 nm or less, very preferably 20 nm or less, and particularly preferably 15 nm or less. In addition, since an extremely narrow band spectrum may not be able to achieve desired characteristics unless many types of light emitting elements are mounted in the light emitting device, the full width at half maximum of the semiconductor light emitting element used in the long wavelength region is 2 nm or more. Is preferable, 4 nm or more is more preferable, 6 nm or more is very preferable, and 8 nm or more is particularly preferable.

  In the long wavelength region, since the band gap of the GaAs substrate is smaller than the band gap of the material forming the active layer structure, light in the emission wavelength region is absorbed. For this reason, it is preferable that the thickness of the substrate is thin, and it is preferable that the substrate is completely removed.

It is preferable that the full width at half maximum of the phosphor material in the long wavelength region used in the light emitting device or the illumination method of the present invention is narrow. From this viewpoint, the full width at half maximum of the emission spectrum of the phosphor material used in the long wavelength region when excited at room temperature is preferably 130 nm or less, more preferably 110 nm or less, very preferably 90 nm or less, and particularly 70 nm or less. Is preferred. In addition, since an extremely narrow band spectrum may not be able to realize desired characteristics unless many types of light emitting elements are mounted in the light emitting device, the full width at half maximum of the phosphor material used in the long wavelength region is 2 nm or more. Is preferable, 4 nm or more is more preferable, 6 nm or more is very preferable, and 8 nm or more is particularly preferable.
In the phosphor material in the long wavelength region, the peak wavelength may be close to 630 nm when a light emitting device is manufactured as a unit with other materials in consideration of both D _uv controllability and radiation efficiency. Highly preferred. That is, in the present invention, a phosphor material having an emission peak in a long wavelength region from Λ3 (590 nm) to 780 nm preferably has a peak between 590 nm and 600 nm, and has a peak at about 600 nm to 780 nm. It is more preferable that the peak wavelength is close to 630 nm. In particular, a phosphor material having a peak wavelength of 620 nm to 655 nm is very preferable.

As a specific example of the phosphor material in the long wavelength region used in the light emitting device or illumination method of the present invention, any phosphor material satisfying the full width at half maximum can be preferably used. Specific examples thereof include phosphors having Eu ²⁺ as an activator and based on a crystal made of alkaline earth silicon nitride, α sialon or alkaline earth silicate. This type of red phosphor can usually be excited using ultraviolet to blue semiconductor light emitting devices. Specific examples of an alkaline earth silicon nitride crystal as a base include phosphors represented by (Ca, Sr, Ba, Mg) AlSiN ₃ : Eu and / or (Ca, Sr, Ba) AlSiN ₃ : Eu (This is called SCASN phosphor), (CaAlSiN ₃ ) _1-x (Si ₂ N ₂ O) _x : Eu (where x is 0 <x <0.5) (this is CASON) referred to as _{phosphor), (Sr, Ca, Ba} ) 2 Al x Si 5-x O x N 8-x: phosphor represented by Eu (provided that _{0 ≦ x ≦ 2), Eu} y (Sr, Ca, _{Ba) 1-y: Al 1} + x Si 4-x O x N 7-x ( except 0 ≦ x <phosphor represented by 4,0 ≦ y <0.2) can be mentioned.

In addition, an Mn ⁴⁺ activated fluoride complex phosphor is also included. The Mn ⁴⁺ activated fluoride complex phosphor is a phosphor using Mn ⁴⁺ as an activator and an alkali metal, amine or alkaline earth metal fluoride complex salt as a base crystal. Fluoride complexes that form host crystals include those whose coordination center is a trivalent metal (B, Al, Ga, In, Y, Sc, lanthanoid), and tetravalent metal (Si, Ge, Sn, Ti, Zr, Re, Hf) and pentavalent metals (V, P, Nb, Ta), and the number of fluorine atoms coordinated around them is 5-7.

Preferred ^{Mn 4+} -activated fluoride complex phosphor, the alkali metal hexafluoro complex salt as host crystals _{A 2 + x M y Mn z} F n (A is Na and / or K; M is Si and Al; -1 ≦ x ≦ 1, 0.9 ≦ y + z ≦ 1.1, 0.001 ≦ z ≦ 0.4, and 5 ≦ n ≦ 7). Particularly preferred are those in which A is one or more selected from K (potassium) or Na (sodium) and M is Si (silicon) or Ti (titanium), for example, K ₂ SiF ₆ : Mn (this Is called KSF phosphor), and K ₂ Si _1-x Na _x Al _x F ₆ : Mn, K ₂ TiF ₆ : Mn in which a part of this constituent element (preferably 10 mol% or less) is substituted with Al and Na. (This is called a KSNAF phosphor).

In addition, a phosphor represented by the following general formula (7) and a phosphor represented by the following general formula (7) ′ are also included.
_{(La 1-x-y,} Eu x, Ln y) 2 O 2 S (7)
(In the general formula (7), x and y represent numbers satisfying 0.02 ≦ x ≦ 0.50 and 0 ≦ y ≦ 0.50, respectively, and Ln represents Y, Gd, Lu, Sc, Sm and Er. Represents at least one trivalent rare earth element.) (The lanthanum oxysulfide phosphor represented by the general formula (7) is referred to as a LOS phosphor).
(K−x) MgO.xAF ₂ .GeO ₂ : yMn ⁴⁺ (7) ′
(In general formula (7) ′, k, x, and y represent numbers satisfying 2.8 ≦ k ≦ 5, 0.1 ≦ x ≦ 0.7, and 0.005 ≦ y ≦ 0.015, respectively. , A is calcium (Ca), strontium (Sr), barium (Ba), zinc (Zn), or a mixture thereof. (The germanate phosphor represented by the general formula (7) is replaced with the MGOF phosphor. Called.)

Among these phosphors, LOS phosphor, MGOF phosphor, KSF phosphor, KSNAF phosphor, SCASN phosphor, CASON phosphor, (Sr, Ca, Ba) ₂ Si ₅ N ₈ : Eu phosphor, (Sr , Ca, Ba) AlSi ₄ N ₇ phosphor and the like can be preferably exemplified.

In the light emitting device or the illumination method of the present invention, there is no particular limitation on the material for appropriately controlling the spectral distribution of the light emitting device. However, it is very preferable that the light emitting device to be embodied is as follows.
A purple LED (with a peak wavelength of about 395 nm to 420 nm) is used as a light emitting element in a short wavelength region, and at least selected from among SBCA, SCA, and BAM that are relatively narrow band phosphors as a light emitting element in a short wavelength region 1 or more are included in the light source, and at least one or more selected from β-SiAlON, BSS, BSON, and G-BAM, which are relatively narrow-band phosphors as light emitting elements in the intermediate wavelength region, are included in the light source, It is preferable that at least one or more selected from among CASON, SCASN, LOS, KSF, and KSNAF is included in the light source as the light emitting element in the long wavelength region.
Furthermore, it is as follows.
A violet LED (with a peak wavelength of about 395 nm to 420 nm) is used as a first light emitting element in a short wavelength region, and a SBCA, which is a relatively narrow band phosphor, is incorporated in a light source as a second light emitting element in a short wavelength region. It is very preferable to use β-SiAlON, which is a relatively narrow-band phosphor, as the first light emitting element in the wavelength region, and to use CASON as the first light emitting element in the long wavelength region.
In addition, a purple LED (with a peak wavelength of about 395 nm to 420 nm) is used as the first light emitting element in the short wavelength region, and an SCA that is a relatively narrow-band phosphor is incorporated in the light source as the second light emitting element in the short wavelength region. It is very preferable to use β-SiAlON, which is a relatively narrow-band phosphor, as the first light emitting element in the intermediate wavelength region, and use CASON as the first light emitting element in the long wavelength region.
In addition, a purple LED (with a peak wavelength of about 395 nm to 420 nm) is used as the first light emitting element in the short wavelength region, and BAM, which is a relatively narrow band phosphor, is incorporated in the light source as the second light emitting element in the short wavelength region. It is very preferable to use BSS, which is a relatively narrow-band phosphor, as the first light emitting element in the intermediate wavelength region, and to use CASON as the first light emitting element in the long wavelength region.
On the other hand, a blue-violet LED (peak wavelength is about 420 nm to 455 nm) and / or a blue LED (peak wavelength is about 455 nm to 485 nm) is a light emitting element in a short wavelength region, and a relatively narrow band fluorescence is used as a light emitting element in an intermediate wavelength region. At least one or more selected from β-SiAlON, BSS, BSON, and G-BAM, which are the body, are included in the light source, and are selected from CASON, SCASN, LOS, KSF, and KSNAF as light emitting elements in the long wavelength region It is preferable that at least one or more of these be included in the light source.
Furthermore, it is as follows.
A blue-violet LED (with a peak wavelength of about 420 nm to 455 nm) and / or a blue LED (with a peak wavelength of about 455 nm to 485 nm) is used as a light emitting element in a short wavelength region and a relatively narrow band as a first light emitting element in an intermediate wavelength region. It is very preferable to use BCAS, which is a phosphor, and SCASN as the first light emitting element in the long wavelength region.
A blue-violet LED (with a peak wavelength of about 420 nm to 455 nm) and / or a blue LED (with a peak wavelength of about 455 nm to 485 nm) is used as a light emitting element in a short wavelength region and a relatively narrow band as a first light emitting element in an intermediate wavelength region. It is very preferable to use β-SiAlON, which is a phosphor, and CASON as the first light emitting element in the long wavelength region.
A blue-violet LED (with a peak wavelength of about 420 nm to 455 nm) and / or a blue LED (with a peak wavelength of about 455 nm to 485 nm) is used as a light emitting element in a short wavelength region and a relatively narrow band as a first light emitting element in an intermediate wavelength region. It is very preferable to use β-SiAlON which is a phosphor, use CASON as the first light emitting element in the long wavelength region, and use KSF or KSNAF as the second light emitting element in the long wavelength region.
A blue-violet LED (with a peak wavelength of about 420 nm to 455 nm) and / or a blue LED (with a peak wavelength of about 455 nm to 485 nm) is used as a light emitting element in a short wavelength region and a relatively narrow band as a first light emitting element in an intermediate wavelength region. It is very preferable to use β-SiAlON, which is a phosphor, and SCASN as the first light emitting element in the long wavelength region.
A blue-violet LED (with a peak wavelength of about 420 nm to 455 nm) and / or a blue LED (with a peak wavelength of about 455 nm to 485 nm) is used as a light emitting element in a short wavelength region and a relatively narrow band as a first light emitting element in an intermediate wavelength region. It is very preferable to use β-SiAlON which is a phosphor, use SCASN as the first light emitting element in the long wavelength region, and use KSF or KSNAF as the second light emitting element in the long wavelength region.

  The combination of these light emitting elements is very convenient for realizing the appearance of the color and the object that the subject has preferred in the visual experiment, such as the peak wavelength position and the full width at half maximum of each light emitting element.

、
ΔＣ_ｎ、（ΔＣ_ｍａｘ−ΔＣ_ｍｉｎ）も、上記記載の発光要素を用いると所望の値に設定しやすくなるため、好ましい。 In the illumination method or the light-emitting device of the present invention, when the light-emitting element (light-emitting material) described so far is used, the index A _cg , the radiation efficiency K (lm / W), D _{uv, and the} like can be easily set to desired values. Therefore, it is preferable. Further, regarding the light as a color stimulus, regarding the difference between the color appearance of the 15 color chart when the illumination by the light emitting device is assumed and the color appearance when the illumination with the calculation reference light is assumed. | Δh _n |,

,
ΔC _n and (ΔC _max −ΔC _min ) are also preferable when the above-described light-emitting element is used because it is easy to set a desired value.

Various means are conceivable for reducing D _uv from 0 to an appropriate negative value. For example, assuming a light-emitting device having one light-emitting element in each of the three wavelength regions, the light-emitting position of the light-emitting element in the long-wavelength region is moved further to the short-wavelength side. Further, it is possible to shift the light emission position of the light emitting element in the intermediate wavelength region from 555 nm, for example, to move to the longer wavelength side. Furthermore, the relative light emission intensity of the light emitting element in the short wavelength region is increased, the relative light emission intensity of the light emitting element in the long wavelength region is increased, the relative light emission intensity of the light emitting element in the intermediate wavelength region is decreased, etc. Is possible. At this time, in order to change D _uv without changing CCT, the light emitting position of the light emitting element in the short wavelength region is moved to the short wavelength side, and the light emitting position of the light emitting element in the long wavelength region is changed. What is necessary is just to perform moving to the long wavelength side simultaneously. Further, in order to change D _uv to the positive side, an operation reverse to the above description may be performed.

Further, for example, assuming a light emitting device having two light emitting elements in each of the three wavelength regions, and reducing D _uv , for example, on the relatively short wavelength side of two light emitting elements in the short wavelength region. It is also possible to increase the relative intensity of a certain light emitting element, increase the relative intensity of a light emitting element on the relatively long wavelength side of two light emitting elements in the superwavelength region, and the like. In order to reduce D _uv without changing the CCT at this time, the relative intensity of the light emitting element on the relatively short wavelength side of the two light emitting elements in the short wavelength region is increased, and The relative intensity of the light emitting elements on the relatively long wavelength side of the two light emitting elements in the wavelength region may be increased at the same time. Further, in order to change D _uv to the positive side, an operation reverse to the above description may be performed.

、
ΔＣ_ｎ、（ΔＣ_ｍａｘ−ΔＣ_ｍｉｎ）を変化させるための手段としては、特にΔＣ_ｎを増加させるためには、Ｄ_ｕｖを所望の値となるように分光分布を全体を調整したうえで、以下のようなことが可能である。各発光要素の半値全幅を狭い材料に置換し、スペクトル形状として各発光要素間を適切に分離する、各発光要素のスペクトル中に凹凸を形成すべく、照明光源、照明器具等の中に所望の波長を吸収するフィルターを設置する、発光装置中にさらに狭帯域な発光をする発光要素を追加搭載する等のことを行えばよい。 On the other hand, | Δh _n |, concerning the difference between the color appearance of the 15 color chart when the illumination by the light emitting device is assumed and the color appearance when the illumination with the calculation reference light is assumed.

,
As means for changing ΔC _n , (ΔC _max −ΔC _min ), in particular, in _order to increase ΔC _n , the spectral distribution is adjusted as a whole so that D _uv becomes a desired value. Is possible. Replace the full width at half maximum of each light-emitting element with a narrow material, and separate each light-emitting element as a spectral shape appropriately. In order to form irregularities in the spectrum of each light-emitting element, a desired light source, lighting fixture, etc. A filter that absorbs the wavelength may be installed, or a light emitting element that emits light in a narrower band may be additionally mounted in the light emitting device.

The control element of the present invention is a passive element that does not have an amplification function by itself, and is suitable for light emitted from a light emitting element or a light emitting device having a relatively low processing degree in a main radiation direction. There is no particular limitation as long as intensity modulation for each wavelength can be applied in such a range and a light-emitting device with a high degree of processing can be constructed. For example, examples of the control element of the present invention include passive devices such as a reflection mirror, an optical filter, and various optical lenses. Further, the control element of the present invention may be a light-absorbing material that is dispersed in the sealing material of the package LED and gives intensity modulation for each wavelength within an appropriate range. However, the control element does not include a light-emitting element, a reflection mirror, an optical filter, a light-absorbing material, or the like that gives only intensity modulation with a small wavelength dependency to light emitted from a light-emitting device having a relatively low degree of processing.
The control element of the present invention preferably reduces the relative spectral intensity of light having a relatively high energy wavelength component such as ultraviolet, near ultraviolet, violet, and blue-violet from the light emitting element. This is because these wavelength regions are likely to cause discoloration, deterioration, corrosion, deterioration, and the like of the illumination object as compared with light irradiation in other wavelength regions. In addition, it is preferable to reduce the relative spectral intensity of light having a wavelength component that can be thermal radiation such as near infrared, middle infrared, and far infrared from the light emitting element. This is also because these wavelength regions are more likely to cause alteration, corrosion, deterioration, etc. of the illumination object as compared with light irradiation in other wavelength regions.

The control element of the present invention preferably absorbs or reflects light in the λ (nm) ≦ 450 nm region, more preferably in the λ (nm) ≦ 410 nm region, in a direction different from the main radiation direction of the light emitting device. .
Further, the control element of the present invention preferably absorbs light in the 710 nm ≦ λ (nm) region, more preferably 750 nm ≦ λ (nm) region, or reflects it in a direction different from the main radiation direction of the light emitting device. Is preferred.
The control element of the present invention may have a function of condensing and / or diffusing light emitted from the light emitting element, for example, a concave lens, a convex lens, a Fresnel lens, and the like.

  As described above, the present invention is natural as a wide variety of illumination objects having various hues in an illuminance range of 150 lx to about 5000 lx are viewed in a high-illuminance environment exceeding 10,000 lx such as outdoors. For lighting objects that are vivid, highly visible, comfortable, and have a color appearance, but are also concerned about secondary effects of light irradiation, a light-emitting device that suppresses such secondary effects The realization method is clarified. In particular, each hue can be naturally vivid, and at the same time, a white object can be perceived as whiter than the experimental reference light.

Further, in the light emitting device of the present invention, means for making a natural, lively, highly visible, comfortable, and colored appearance as seen in a high illumination environment is emitted in the main radiation direction. A light emitting device having an appropriate range of D _uv obtained from the spectral distribution of light, and a light emitting device having an index A _cg in an appropriate range.

  In other words, the present invention is a light emitting device in which the light emitted from the light emitting element is subjected to intensity modulation with respect to an appropriate wavelength by the control element, and the light emitted from the light emitting device satisfies the condition 1-3. Any device may be used as long as the device is used. For example, the device may be a single illumination light source or an illumination module in which at least one of the light sources is mounted on a heat sink or the like. The lighting fixture which provided the circuit etc. may be sufficient. Furthermore, it may be an illumination system having a mechanism that collects at least a light source, a module, a fixture, and the like and supports them at least.

、
ΔＣ_ｎ、（ΔＣ_ｍａｘ−ΔＣ_ｍｉｎ）等の指標を適切な範囲にすることである。 In the lighting method of the present invention, the means for making a natural, lively, highly visible, comfortable, and colored appearance as seen in a high-light environment is the light at the position of the lighting object. D _uv is in an appropriate range, and the color appearance of the 15 color chart assuming illumination with the light and the color of the 15 color chart assuming illumination with the reference light for calculation are used. | Δh _n | regarding the difference from appearance,

,
An index such as ΔC _n and (ΔC _max −ΔC _min ) is set to an appropriate range.

、
ΔＣ_ｎ、（ΔＣ_ｍａｘ−ΔＣ_ｍｉｎ）、Ｄ_{ｕｖＳＳＬ}等が適切な範囲となっている光を照明対象物に照射する照明方法であり、本発明の照明方法に用いる発光装置としては、このような照明が可能な装置であれば、どのような構成をとる装置であっても構わない。当該装置は、たとえば照明光源単体であっても、当該光源を放熱板等の上に少なくとも１以上搭載している照明用モジュールであっても、当該光源あるいはモジュールにレンズ、反射機構、駆動用電気回路等を付与した照明器具であっても良い。さらには、光源単体、モジュール単体、器具単体等を集合させ、少なくともこれらを支持する機構を有する照明システムであってもよい。 In other words, the illumination method of the present invention includes light emitted from the semiconductor light emitting element as a component in the spectral distribution, and | Δh _n |,

,
ΔC _n , (ΔC _max −ΔC _min ), _DuvSSL is an illumination method for irradiating an illumination object with light in an appropriate range. Any device may be used as long as it can illuminate. For example, the device may be a single illumination light source or an illumination module in which at least one of the light sources is mounted on a heat sink or the like. The lighting fixture which provided the circuit etc. may be sufficient. Furthermore, it may be an illumination system having a mechanism that collects at least a light source, a module, a fixture, and the like and supports them at least.

The radiometric, photometric and colorimetric characteristics of the light emitting device of this example are summarized in Table 8, and the color appearance of the illumination object is very good overall. It was.
Therefore, the light-emitting device of the present invention can realize a light-emitting device that does not deteriorate the illumination object and has good color appearance.

DESCRIPTION OF SYMBOLS 1 Case 2 LED chip 2a Blue LED chip 2b Green LED chip 2c Red LED chip 2d Thermal radiation filament 3 Package 4 Phosphor 5 Cut filter (control element)
6 Encapsulant 10 Package LED (Low-light-emitting device)
11 Incandescent light bulb (light emitting device of medium processing level)
20 LED light bulb with filter (light emitting device with high degree of processing)
30 Lighting system (light emitting device with higher processing degree)

  The light-emitting device or the lighting method of the illumination light source, the lighting fixture, and the lighting system of the present invention has a very wide application field, and can be used without being limited to a specific application. However, in view of the features of the illumination method or the light-emitting device of the present invention, application to the following fields is preferable.

For example, when illuminated by the light-emitting device or illumination method of the present invention, white is whiter and naturally even with substantially the same CCT and substantially the same illuminance as compared with the conventional illumination method or light-emitting device. Looks comfortable. Furthermore, it becomes easy to visually recognize the brightness difference between achromatic colors such as white, gray, and black.
For this reason, for example, black characters on general white paper are easy to read. Taking advantage of such features, it is preferable to apply it to work lights such as reading lights, learning desk lights, and office lights. In addition, depending on the work content, inspect the appearance of fine parts in factories, etc., identify colors close to fabrics, etc., check colors for fresh meat freshness check, product inspection against limit samples However, when illuminated by the illumination method of the present invention, it is easy to identify colors in adjacent hues, and a comfortable working environment as if in a high illumination environment can be realized. Therefore, it is preferable to adapt to work illumination from such a viewpoint.

  Furthermore, it is also preferable to apply to medical illumination such as a light source for use in a surgical operation, a gastric camera, etc., because the color discrimination ability is improved. This is because arterial blood is bright red because it contains a lot of oxygen, whereas venous blood is dark red because it contains a lot of carbon dioxide. Although both are the same red color, but their saturations are different, it is expected that arterial blood and venous blood will be readily discriminated by the device or illumination method of the present invention that realizes good color appearance (saturation). . In addition, in color image information such as an endoscope, it is clear that good color display has a great influence on diagnosis, and it is expected that a normal site and a lesion site can be easily distinguished. For the same reason, it can be suitably used as an illumination method in industrial equipment such as an image discriminator for products.

When illuminated by the light emitting device or illumination method of the present invention, even if the illuminance is about several thousand Lx to several hundred Lx, purple, blue purple, blue, blue green, green, yellow green, yellow, yellow red Realize the natural appearance of most colors, such as red, purple, and sometimes all colors, as seen under tens of thousands of lx, such as under sunny day outdoors Is done. In addition, the skin color of subjects (Japanese people), various foods, clothing, wood colors, and the like, which have intermediate saturation, have natural colors that many subjects feel more preferable.
Therefore, if the light-emitting device or lighting method of the present invention is applied to general lighting for home use, the food looks fresh and appetizing, it is easy to read newspapers and magazines, etc., and the visibility of steps, etc. It is thought that it will also increase safety in the home. Therefore, it is preferable to apply the present invention to household lighting. Moreover, it is also preferable as illumination for exhibits such as clothing, food, cars, bags, shoes, decorations, furniture, etc., and illumination that can be visually recognized from the periphery is possible.
It is also preferable for illumination of articles such as cosmetics whose subtle color differences are decisive for purchase. When used as lighting for exhibits such as white dresses, it is easy to see subtle color differences, such as bluish white and cream-like white, even with the same white, so select the color you want It becomes possible. Furthermore, it is also suitable as lighting for directing in a wedding hall, a theater, etc., a pure white dress or the like looks pure white, and a kimono such as a kabuki or a dress is clearly visible. Furthermore, the skin color is also particularly preferable. Further, when used as lighting for a beauty salon, when hair is color-treated, it becomes possible to have a color that does not wrinkle when viewed outdoors, and it is possible to prevent excessive dyeing or insufficient dyeing.

In particular, the light-emitting device or illumination method of the present invention reduces the relative spectral intensity of light having a relatively high energy wavelength component such as ultraviolet, near-ultraviolet, purple, and blue-violet from the light-emitting element by the control element. Therefore, it is possible to reduce fading, deterioration, corrosion, deterioration, etc. of lighting objects such as clothing and food. In addition, the light-emitting device or the illumination method of the present invention reduces the relative spectral intensity of light having a wavelength component that can be heat radiation from the light-emitting element such as near infrared, mid-infrared, far-infrared, etc. It is possible to reduce alteration, corrosion, deterioration, etc. of the lighting object such as.

  In addition, since white appears whiter, achromatic colors can be easily identified, and chromatic colors also become natural vivid, so in a limited space where many types of activities are performed. It is also suitable as a light source. For example, in a passenger seat on an aircraft, reading is done, work is done, and food is also served. The situation is similar for trains, long-distance buses, and the like. The present invention can be suitably used as such interior lighting for transportation.

In addition, white looks more white, making it easy to identify achromatic colors, and chromatic colors are also naturally vivid, so lighting in natural colors as if viewing paintings at museums etc. outdoors Therefore, the present invention can be suitably used as an illumination for art works.

  On the other hand, this invention can be utilized suitably also as illumination for elderly people. That is, even when fine characters are difficult to see under normal illuminance, steps, etc. are difficult to see, by applying the illumination method or the light emitting device of the present invention, between achromatic colors or between chromatic colors. Since identification becomes easy, these problems can be solved. Therefore, it can be suitably used for lighting in public facilities used by an unspecified number of people such as nursing homes, hospital waiting rooms, bookstores, and libraries.

  Furthermore, the light-emitting device or illumination method of the present invention can be suitably used in applications that ensure visibility by adapting to an illumination environment that tends to have relatively low illuminance due to various circumstances.

  For example, it is also preferable to apply to street lights, car headlights, and foot lamps to improve various visibility compared to the case of using a conventional light source.

Claims (62)

A light emitting device including a light emitting element and a control element,
Let the wavelength be λ (nm),
The total radiant flux spectral distribution emitted from the light emitting element is Φ _elm (λ), and the wavelength λ giving the maximum total radiant flux spectral intensity Φ _elmmax within the defined wavelength range is λ _elmmax (nm), Φ _elm (λ) _Is the relative total radiant flux spectral distribution of the light-emitting element divided by Φ _elmmax , and Φ _elmrel (λ),
The relative spectral distribution of the light emitting device obtained by dividing the spectral distribution of the light emitted from the light emitting device in the main radiation direction by φ _SSL (λ) and φ _SSL (λ) by φ _SSL (λ _elmmax ) is φ _SSLrel (λ). When
The light expressed by Φ _elmrel (λ) and the light expressed by φ _SSLrel (λ) satisfy both the conditions 1 and 2 by the control element, and the light expressed by φ _SSLrel (λ) is a condition. 3, a light emitting device satisfying the above requirement.
<Condition 1>
In all λ of 530 nm ≦ λ ≦ 580 nm, 0.70 ≦ φ _SSLrel (λ) / Φ _elmrel (λ) ≦ 1.30 holds.
<Condition 2>
At 380 nm ≦ λ ≦ 780 nm,
There _exists λ _satisfying φ _SSLrel (λ) / Φ _elmrel (λ) ≦ 0.97 or 1.03 ≦ φ _SSLrel (λ) / Φ _elmrel (λ).
<Condition 3>
At 380 nm ≦ λ ≦ 780 nm,
The distance D _uvSSL from the black body radiation locus defined by ANSI C78.377 related to φ _SSLrel (λ) is −0.0350 ≦ D _uvSSL ≦ −0.0040. The light-emitting device according to claim 1, wherein the light-emitting device also satisfies condition 4.
<Condition 4>
0.90 ≦ φ _SSLrel (λ) / Φ _elmrel (λ) ≦ 1.10 holds for all λ of 530 nm ≦ λ ≦ 580 nm. The light-emitting device according to claim 1, wherein the light-emitting device also satisfies condition 5.
<Condition 5>
0.80 ≦ φ _SSLrel (λ) / Φ _elmrel (λ) ≦ 1.20 holds for all λ of 495 nm ≦ λ ≦ 590 nm. The light-emitting device according to claim 1, wherein the light-emitting device also satisfies condition 6.
<Condition 6>
At 380 nm ≦ λ ≦ 495 nm,
There _exists λ _satisfying φ _SSLrel (λ) / Φ _elmrel (λ) ≦ 0.70 or 1.30 ≦ φ _SSLrel (λ) / Φ _elmrel (λ). The light-emitting device according to claim 4, wherein the light-emitting device also satisfies condition 7.
<Condition 7>
At 380 nm ≦ λ ≦ 495 nm,
There _exists λ _satisfying φ _SSLrel (λ) / Φ _elmrel (λ) ≦ 0.40 or 1.60 ≦ φ _SSLrel (λ) / Φ _elmrel (λ). 6. The light emitting device according to claim 4 or 5, wherein the light emitting device also satisfies condition 8.
<Condition 8>
At 380 nm ≦ λ ≦ 495 nm,
There _exists λ _satisfying φ _SSLrel (λ) / Φ _elmrel (λ) ≦ 0.10 or 1.90 ≦ φ _SSLrel (λ) / Φ _elmrel (λ). The light-emitting device according to claim 1, wherein the light-emitting device also satisfies condition 9.
<Condition 9>
At 590 nm ≦ λ ≦ 780 nm,
There _exists λ _satisfying φ _SSLrel (λ) / Φ _elmrel (λ) ≦ 0.70 or 1.30 ≦ φ _SSLrel (λ) / Φ _elmrel (λ). The light-emitting device according to claim 7, wherein the light-emitting device also satisfies condition 10. <Condition 10>
At 590 nm ≦ λ ≦ 780 nm,
There _exists λ _satisfying φ _SSLrel (λ) / Φ _elmrel (λ) ≦ 0.40 or 1.60 ≦ φ _SSLrel (λ) / Φ _elmrel (λ). The light-emitting device according to claim 7, wherein the light-emitting device also satisfies the condition 11.
<Condition 11>
At 590 nm ≦ λ ≦ 780 nm,
There _exists λ _satisfying φ _SSLrel (λ) / Φ _elmrel (λ) ≦ 0.10 or 1.90 ≦ φ _SSLrel (λ) / Φ _elmrel (λ).   10. The light emitting device according to claim 1, wherein the control element absorbs or reflects light in a λ (nm) ≦ 450 nm region. 11.   The light-emitting device according to claim 10, wherein the control element absorbs or reflects light in a λ (nm) ≦ 410 nm region in a direction different from a main radiation direction of the light-emitting device.   The light-emitting device according to claim 1, wherein the control element absorbs light in a region of 710 nm ≦ λ (nm) or reflects the light in a direction different from a main radiation direction of the light-emitting device. A light emitting device characterized.   13. The light emitting device according to claim 12, wherein the control element absorbs or reflects light in a region of 750 nm ≦ λ (nm).   The light-emitting device according to any one of claims 1 to 13, wherein the control element has a function of condensing and / or diffusing light emitted from the light-emitting element.   15. The light emitting device according to claim 14, wherein the condensing and / or diffusing function of the control element is realized by at least one function of a concave lens, a convex lens, and a Fresnel lens. The light emitting device according to any one of claims 1 to 15, wherein the light emitting element includes a semiconductor light emitting element. The light-emitting device according to any one of claims 1 to 16, wherein the black-body radiation defined by ANSI C78.377 relates to a total radiant flux spectral distribution Φ _elm (λ) emitted from the light-emitting element. A light emitting device characterized in that a distance D _uvelm from the locus satisfies −0.0350 ≦ D _uvelm ≦ −0.0040. The light-emitting device according to any one of claims 1 to 17,
The reference light spectral distribution selected according to the correlated color temperature T _SSL (K) of the light derived from φ _SSL (λ) is φ _ref (λ), and is emitted from the light emitting device in the radiation direction. The tristimulus values of light (X _SSL , Y _SSL , Z _SSL ) and the reference tristimulus values of light selected according to T _SSL (K) of light emitted from the light emitting device in the radiation direction ( X _ref , Y _ref , Z _ref )
A standard selected according to the normalized spectral distribution S _SSL (λ) of light emitted from the light emitting device in the emission direction and T _SSL (K) of light emitted from the light emission device in the emission direction. The normalized spectral distribution S _ref (λ) of light and the difference ΔS (λ) between these normalized spectral distributions are respectively
S _SSL (λ) = φ _SSL (λ) / Y _SSL
S _ref (λ) = φ _ref (λ) / Y _ref
ΔS (λ) = S _ref (λ) −S _SSL (λ)
And define
Within a range of wavelength 380nm or 780 _nm, the wavelength giving the longest wavelength maximum of the _{S SSL} (lambda) upon the _{λ R (nm), λ S} SSL (λ R) on the longer wavelength side than _R / 2 and There exists a wavelength Λ4,
An index A _cg represented by the following mathematical formula (1) satisfies −360 ≦ A _cg ≦ −10.

The light-emitting device according to any one of claims 1 to 17,
The reference light spectral distribution selected according to the correlated color temperature T _SSL (K) of the light derived from φ _SSL (λ) is φ _ref (λ), and is emitted from the light emitting device in the radiation direction. The tristimulus values of light (X _SSL , Y _SSL , Z _SSL ) and the reference tristimulus values of light selected according to T _SSL (K) of light emitted from the light emitting device in the radiation direction ( X _ref , Y _ref , Z _ref )
A standard selected according to the normalized spectral distribution S _SSL (λ) of light emitted from the light emitting device in the emission direction and T _SSL (K) of light emitted from the light emission device in the emission direction. The normalized spectral distribution S _ref (λ) of light and the difference ΔS (λ) between these normalized spectral distributions are respectively
S _SSL (λ) = φ _SSL (λ) / Y _SSL
S _ref (λ) = φ _ref (λ) / Y _ref
ΔS (λ) = S _ref (λ) −S _SSL (λ)
And define
Within a range of wavelength 380nm or 780 _nm, the wavelength giving the longest wavelength maximum of the _{S SSL} (lambda) upon the _{λ R (nm), λ S} SSL (λ R) on the longer wavelength side than _R / 2 and There is no wavelength Λ4,
An index A _cg represented by the following mathematical formula (2) satisfies −360 ≦ A _cg ≦ −10.

The light-emitting device according to claim 18 or 19,
The light emitted from the light emitting device in the radiation direction satisfies the following (1) and (2).
(1) CIE 1976 L ^* a ^* b ^{* of the following} 15 modified Munsell color charts from # 01 to # 15 when mathematically assuming illumination by light emitted in the radiation direction from the light emitting device
The a ^* value and b ^* value in the color space are a ^* _nSSL and b ^* _nSSL (where n is a natural number from 1 to 15, respectively)
CIE 1976 of the 15 kinds of modified Munsell color charts when the illumination with the reference light selected according to the correlated color temperature T _SSL (K) of the light emitted in the radiation direction is mathematically assumed.
When the a ^* value and b ^* value in the L ^* a ^* b ^* color space are a ^* _nref and b ^* _nref (where n is a natural number from 1 to 15), the saturation difference ΔC _n is −3.8. ≦ ΔC _n ≦ 18.6 (n is a natural number from 1 to 15)
And the average saturation difference represented by the following formula (3) satisfies the following formula (4):

When the maximum value of the saturation difference is ΔC _max and the minimum value of the saturation difference is ΔC _min , the difference ΔC _max −ΔC _min between the maximum value of the saturation difference and the minimum value of the saturation difference is 2.8 ≦ (ΔC _max −ΔC _min ) ≦ 19.6
Meet.
Note that ΔC _n = √ {(a ^* _nSSL ) ² + (b ^* _nSSL ) ² } −√ {(a ^* _nref ) ² + (b ^* _nref ) ² }.
15 types of modified Munsell color chart # 01 7.5 P 4/10
# 02 10 PB 4/10
# 03 5 PB 4/12
# 04 7.5 B 5/10
# 05 10 BG 6/8
# 06 2.5 BG 6/10
# 07 2.5 G 6/12
# 08 7.5 GY 7/10
# 09 2.5 GY 8/10
# 10 5 Y 8.5 / 12
# 11 10 YR 7/12
# 12 5 YR 7/12
# 13 10 R 6/12
# 14 5 R 4/14
# 15 7.5 RP 4/12
(2) The hue angle in the CIE 1976 L ^* a ^* b ^* color space of the above 15 types of modified Munsell color _charts when the illumination by the light emitted from the light emitting device in the radiation direction is mathematically assumed is θ _nSSL. (Degree) (where n is a natural number from 1 to 15)
CIE 1976 of the 15 kinds of modified Munsell color charts when the illumination with the reference light selected according to the correlated color temperature T _SSL (K) of the light emitted in the radiation direction is mathematically assumed.
When the hue angle in the L ^* a ^* b ^* color space is θ _nref (degrees) (where n is a natural number from 1 to 15), the absolute value of the hue angle difference | Δh _n | is 0 ≦ | Δh _n | ≦ 9.0 (degrees) (n is a natural number from 1 to 15)
Meet.
However, it is set as _{( DELTA) hn} = (theta) _{nSSL- (} theta) _nref . The light-emitting device according to any one of claims 18 to 20,
The light emitted from the light emitting device in the radiation direction has a radiation efficiency K (lm / W) in the range of 380 nm to 780 nm derived from the spectral distribution φ _SSL (λ), 180 (lm / W) ≦ K (Lm / W) ≦ 320 (lm / W)
A light emitting device characterized by satisfying the above. 21. The light emitting device according to claim 20, wherein the absolute value of the hue angle difference | Δh _n | is 0.0003 ≦ | Δh _n | ≦ 8.3 (degrees) (n is a natural number of 1 to 15).
A light emitting device characterized by satisfying the above. 21. The light emitting device according to claim 20, wherein an average of the saturation difference represented by the general formula (3) satisfies the following formula (4) ′.

(4) ' 21. The light emitting device according to claim 20, wherein the saturation difference ΔC _n is −3.4 ≦ ΔC _n ≦ 16.8 (n is a natural number from 1 to 15).
A light emitting device characterized by satisfying the above. 21. The light emitting device according to claim 20, wherein a difference ΔC _max −ΔC _min between the maximum value of the saturation difference and the minimum value of the saturation difference is 3.2 ≦ (ΔC _max −ΔC _min ). ≦ 17.8
A light emitting device characterized by satisfying the above. The light-emitting device according to any one of claims 18 to 25,
The light emitted from the light emitting device in the radiation direction has a distance D _uvSSL from the black body radiation locus of −0.0250 ≦ D _uvSSL ≦ −0.0100.
A light emitting device characterized by satisfying the above. 27. The light emitting device according to any one of claims 18 to 26, wherein an index A _cg represented by the formula (1) or (2) is −322 ≦ A _cg ≦ −12.
A light emitting device characterized by satisfying the above. The light-emitting device according to any one of claims 18 to 27,
The light emitted from the light emitting device in the radiation direction has a radiation efficiency K (lm / W) in a wavelength range of 380 nm or more and 780 nm or less derived from the spectral distribution φ _SSL (λ).
206 (lm / W) ≦ K (lm / W) ≦ 288 (lm / W)
A light emitting device characterized by satisfying the above. A light emitting device according to any one of claims 18 to 28, wherein the correlated color temperature _{T SSL} (K) is _{2550 (K) ≦ T SSL (} K) ≦ 5650 (K)
A light emitting device characterized by satisfying the above.   30. The light emitting device according to any one of claims 18 to 29, wherein the illuminance at which the light emitted from the light emitting device in the radiation direction illuminates the object is 150 lx or more and 5000 lx or less. Light emitting device.   31. The light emitting device according to any one of claims 18 to 30, wherein the light emitting device emits light emitted from one or more kinds of light emitting elements to six kinds or less in the radiation direction. .   32. The light emitting device according to claim 18, wherein the light emitting device includes a semiconductor light emitting element as a light emitting element, and a peak wavelength of an emission spectrum of the semiconductor light emitting element is not less than 380 nm and less than 495 nm. And a full width at half maximum of 2 nm to 45 nm.   33. The light emitting device according to claim 32, wherein a peak wavelength of an emission spectrum of the semiconductor light emitting element is not less than 395 nm and less than 420 nm.   33. The light emitting device according to claim 32, wherein a peak wavelength of an emission spectrum of the semiconductor light emitting element is 420 nm or more and less than 455 nm.   33. The light emitting device according to claim 32, wherein a peak wavelength of an emission spectrum of the semiconductor light emitting element is not less than 455 nm and less than 485 nm. 32. The light emitting device according to any one of claims 18 to 31, wherein the light emitting device includes a semiconductor light emitting element as a light emitting element, and a peak wavelength of an emission spectrum of the semiconductor light emitting element is 49.
A light emitting device having a width of 5 nm or more and less than 590 nm and a full width at half maximum of 2 nm or more and 75 nm or less.   32. The light-emitting device according to claim 18, wherein the light-emitting device includes a semiconductor light-emitting element as a light-emitting element, and a peak wavelength of an emission spectrum of the semiconductor light-emitting element is not less than 590 nm and less than 780 nm. And a full width at half maximum of 2 nm to 30 nm.   32. The light emitting device according to claim 18, wherein the light emitting device includes a semiconductor light emitting element as a light emitting element, and the semiconductor light emitting element includes a sapphire substrate, a GaN substrate, a GaAs substrate, and a GaP substrate. A light-emitting device produced on any substrate selected from the group.   32. The light emitting device according to any one of claims 18 to 31, wherein the light emitting device includes a semiconductor light emitting element as a light emitting element, the semiconductor light emitting element is formed on a GaN substrate or a GaP substrate, and A light-emitting device having a substrate thickness of 100 μm to 2 mm.   33. The light emitting device according to any one of claims 18 to 32, wherein the light emitting device includes a semiconductor light emitting element as a light emitting element, the semiconductor light emitting element is formed on a sapphire substrate or a GaAs substrate, and is a semiconductor. A light-emitting device, wherein the light-emitting element is peeled from the substrate.   36. The light emitting device according to any one of claims 18 to 35, comprising a phosphor as a light emitting element.   42. The light-emitting device according to claim 41, wherein the phosphor includes one to five phosphors having different emission spectra.   43. The light-emitting device according to claim 41 or claim 42, wherein the phosphor has a peak wavelength of a single emission spectrum of 380 nm or more and less than 495 nm when photoexcited at room temperature, and a full width at half maximum of 2 nm or more and 90 nm. A light-emitting device comprising the following phosphor. 44. The light-emitting device according to claim 43, wherein the phosphor is a phosphor represented by the following general formula (5), a phosphor represented by the following general formula (5) ′, (Sr, Ba) ₃ MgSi A light emitting device including one or more selected from the group consisting of ₂ O ₈ : Eu ²⁺ and (Ba, Sr, Ca, Mg) Si ₂ O ₂ N ₂ : Eu.
(Ba, Sr, Ca) MgAl ₁₀ O ₁₇ : Mn, Eu (5)
_{Sr a Ba b Eu x (PO} 4) c X d (5) '
(In the general formula (5) ′, X is Cl. Also, c, d and x are 2.7 ≦ c ≦ 3.3, 0.9 ≦ d ≦ 1.1, 0.3 ≦ x ≦. (In addition, a and b satisfy the condition of a + b = 5-x and 0 ≦ b / (a + b) ≦ 0.6.)   43. The light-emitting device according to claim 41 or claim 42, wherein the phosphor has a peak wavelength of a single emission spectrum of 495 nm to less than 590 nm when photoexcited at room temperature, and a full width at half maximum of 2 nm to 130 nm. A light-emitting device comprising the following phosphor. A light emitting device according to claim 45, wherein the phosphor is _{Si 6-z Al z O z} N 8-z:
Eu (provided that 0 <z <4.2), a phosphor represented by the following general formula (6), a phosphor represented by the following general formula (6) ′, and SrGaS ₄ : Eu ²⁺ A light emitting device comprising one or more of the above.
_{(Ba a Ca b Sr c Mg} d Eu x) SiO 4 (6)
(In the general formula (6), a, b, c, d and x are a + b + c + d + x = 2, 1.0 ≦ a ≦ 2.0, 0 ≦ b <0.2, 0.2 ≦ c ≦ 0.8, 0 ≦ d <0.2
And 0 <x ≦ 0.5. )
Ba _1-xy Sr _x Eu _y Mg _1-z Mn _z Al ₁₀ O ₁₇ (6) ′
(In the general formula (6) ′, x, y, and z satisfy 0.1 ≦ x ≦ 0.4, 0.25 ≦ y ≦ 0.6, and 0.05 ≦ z ≦ 0.5, respectively.)   43. The light-emitting device according to claim 41 or claim 42, wherein the phosphor has a single emission spectrum peak wavelength of 590 nm or more and less than 780 nm when photoexcited at room temperature, and a full width at half maximum of 2 nm or more and 130 nm. A light-emitting device comprising the following phosphor. 48. The light-emitting device according to claim 47, wherein the phosphor is a phosphor represented by the following general formula (7), a phosphor represented by the following general formula (7) ′, (Sr, Ca, Ba) _{2 Al x Si 5-x O} x N 8-x: Eu ( provided that _{0 ≦ x ≦ 2), Eu} y (Sr, Ca, Ba) 1-y: Al 1 + x Si 4-x O x N 7-x ( However _{0 ≦ x <4,0 ≦ y <} 0.2), K 2 SiF 6: Mn 4+, A 2 + x M y Mn z F n (A is Na and / or K; M is Si and Al; -1 ≦ x ≦ 1 and 0.9 ≦ y + z ≦ 1.1 and 0.001 ≦ z ≦ 0.4 and 5 ≦ n ≦ 7), (Ca, Sr, Ba, Mg) AlSiN ₃ : Eu and / or (Ca, Sr, Ba) AlSiN ₃ : Eu and (CaAlSiN ₃ ) _1-x (Si ₂ N ₂ O) _x : Eu However, x is 1 or more types selected from the group which consists of 0 <x <0.5), The light-emitting device characterized by the above-mentioned.
_{(La 1-x-y,} Eu x, Ln y) 2 O 2 S (7)
(In the general formula (7), x and y represent numbers satisfying 0.02 ≦ x ≦ 0.50 and 0 ≦ y ≦ 0.50, respectively, and Ln represents Y, Gd, Lu, Sc, Sm and Er. Represents at least one trivalent rare earth element)
(K−x) MgO.xAF ₂ .GeO ₂ : yMn ⁴⁺ (7) ′
(In general formula (7) ′, k, x, and y represent numbers satisfying 2.8 ≦ k ≦ 5, 0.1 ≦ x ≦ 0.7, and 0.005 ≦ y ≦ 0.015, respectively. , A is calcium (Ca), strontium (Sr), barium (Ba), zinc (Zn), or a mixture thereof.   32. The light-emitting device according to claim 18, comprising a semiconductor light-emitting element and a phosphor as a light-emitting element, and the semiconductor light-emitting element has an emission spectrum peak wavelength of 395 nm or more and less than 420 nm, The phosphor includes SBCA, β-SiAlON, and CASON.   32. The light-emitting device according to claim 18, comprising a semiconductor light-emitting element and a phosphor as a light-emitting element, and the semiconductor light-emitting element has an emission spectrum peak wavelength of 395 nm or more and less than 420 nm, The phosphor includes SCA, β-SiAlON, and CASON.   51. The light emitting device according to any one of claims 18 to 50, wherein the light emitting device is any one selected from the group consisting of packaged LEDs, LED modules, LED lighting fixtures, and LED lighting systems. Light emitting device. The light-emitting device according to any one of claims 18 to 51, which is used as a home lighting device.   52. The light emitting device according to any one of claims 18 to 51, which is used as an illumination device for an exhibit.   52. The light-emitting device according to any one of claims 18 to 51, which is used as an effect lighting device.   The light-emitting device according to any one of claims 18 to 51, which is used as a medical lighting device. The light-emitting device according to any one of claims 18 to 51, which is used as a work lighting device.   52. The light-emitting device according to any one of claims 18 to 51, which is used as a lighting device for industrial equipment.   52. The light-emitting device according to any one of claims 18 to 51, which is used as a lighting device for transportation interior.   The light-emitting device according to any one of claims 18 to 51, which is used as a lighting device for fine arts.   52. The light-emitting device according to any one of claims 18 to 51, wherein the light-emitting device is used as an elderly lighting device. A method of designing a light emitting device including a light emitting element and a control element,
Let the wavelength be λ (nm),
The total radiant flux spectral distribution emitted from the light emitting element is Φ _elm (λ), and the wavelength λ giving the maximum total radiant flux spectral intensity Φ _elmmax within the defined wavelength range is λ _elmmax (nm), Φ _elm (λ) _Is the relative total radiant flux spectral distribution of the light-emitting element divided by Φ _elmmax , and Φ _elmrel (λ),
The relative spectral distribution of the light emitting device obtained by dividing the spectral distribution of the light emitted from the light emitting device in the main radiation direction by φ _SSL (λ) and φ _SSL (λ) by φ _SSL (λ _elmmax ) is φ _SSLrel (λ). When
The light expressed by Φ _elmrel (λ) and the light expressed by φ _SSLrel (λ) satisfy both the conditions 1 and 2 by the control element, and the light expressed by φ _SSLrel (λ) is a condition. 3 is a method for designing a light emitting device.
<Condition 1>
In all λ of 530 nm ≦ λ ≦ 580 nm, 0.70 ≦ φ _SSLrel (λ) / Φ _elmrel (λ) ≦ 1.30 holds.
<Condition 2>
At 380 nm ≦ λ ≦ 780 nm,
There _exists λ _satisfying φ _SSLrel (λ) / Φ _elmrel (λ) ≦ 0.97 or 1.03 ≦ φ _SSLrel (λ) / Φ _elmrel (λ).
<Condition 3>
At 380 nm ≦ λ ≦ 780 nm,
The distance D _uvSSL from the black body radiation locus defined by ANSI C78.377 related to φ _SSLrel (λ) is −0.0350 ≦ D _uvSSL ≦ −0.0040. An illumination step of illuminating an object with light emitted from a light emitting device including a light emitting element and a control element,
Let the wavelength be λ (nm),
The total radiant flux spectral distribution emitted from the light emitting element is Φ _elm (λ), and the wavelength λ giving the maximum total radiant flux spectral intensity Φ _elmmax within the defined wavelength range is λ _elmmax (nm), Φ _elm (λ) _Is the relative total radiant flux spectral distribution of the light-emitting element divided by Φ _elmmax , and Φ _elmrel (λ),
The relative spectral distribution of the light emitting device obtained by dividing the spectral distribution of the light emitted from the light emitting device in the main radiation direction by φ _SSL (λ) and φ _SSL (λ) by φ _SSL (λ _elmmax ) is φ _SSLrel (λ). When
The light expressed by Φ _elmrel (λ) and the light expressed by φ _SSLrel (λ) satisfy both the conditions 1 and 2 by the control element, and the light expressed by φ _SSLrel (λ) is a condition. 3. An illumination method including an illumination step of illuminating an object with light emitted from the light emitting device satisfying 3.
<Condition 1>
In all λ of 530 nm ≦ λ ≦ 580 nm, 0.70 ≦ φ _SSLrel (λ) / Φ _elmrel (λ) ≦ 1.30 holds.
<Condition 2>
At 380 nm ≦ λ ≦ 780 nm,
There _exists λ _satisfying φ _SSLrel (λ) / Φ _elmrel (λ) ≦ 0.97 or 1.03 ≦ φ _SSLrel (λ) / Φ _elmrel (λ).
<Condition 3>
At 380 nm ≦ λ ≦ 780 nm,
The distance D _uvSSL from the black body radiation locus defined by ANSI C78.377 related to φ _SSLrel (λ) is −0.0350 ≦ D _uvSSL ≦ −0.0040.

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