JP2018156956A5 - - Google Patents
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- JP2018156956A5 JP2018156956A5 JP2018112446A JP2018112446A JP2018156956A5 JP 2018156956 A5 JP2018156956 A5 JP 2018156956A5 JP 2018112446 A JP2018112446 A JP 2018112446A JP 2018112446 A JP2018112446 A JP 2018112446A JP 2018156956 A5 JP2018156956 A5 JP 2018156956A5
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- OAICVXFJPJFONN-UHFFFAOYSA-N phosphorus Chemical compound [P] OAICVXFJPJFONN-UHFFFAOYSA-N 0.000 claims description 28
- 229910052791 calcium Inorganic materials 0.000 claims description 2
- 229910052712 strontium Inorganic materials 0.000 claims description 2
- 230000003595 spectral Effects 0.000 claims 46
- 241001106462 Ulmus Species 0.000 claims 30
- 235000010956 sodium stearoyl-2-lactylate Nutrition 0.000 claims 27
- 230000002596 correlated Effects 0.000 claims 12
- 238000005286 illumination Methods 0.000 claims 8
- 230000005284 excitation Effects 0.000 claims 4
- 239000004065 semiconductor Substances 0.000 claims 4
- 230000005457 Black-body radiation Effects 0.000 claims 2
- 102100001764 ALS2 Human genes 0.000 claims 1
- 101700045037 ALS2 Proteins 0.000 claims 1
- 230000003287 optical Effects 0.000 claims 1
- 239000011575 calcium Substances 0.000 description 2
- CPLXHLVBOLITMK-UHFFFAOYSA-N magnesium oxide Chemical compound [Mg]=O CPLXHLVBOLITMK-UHFFFAOYSA-N 0.000 description 2
- 239000000126 substance Substances 0.000 description 2
- 239000011701 zinc Substances 0.000 description 2
- 229910052691 Erbium Inorganic materials 0.000 description 1
- 229910052688 Gadolinium Inorganic materials 0.000 description 1
- 229910005793 GeO 2 Inorganic materials 0.000 description 1
- 229910052765 Lutetium Inorganic materials 0.000 description 1
- 229910052772 Samarium Inorganic materials 0.000 description 1
- 229910052788 barium Inorganic materials 0.000 description 1
- DSAJWYNOEDNPEQ-UHFFFAOYSA-N barium(0) Chemical compound [Ba] DSAJWYNOEDNPEQ-UHFFFAOYSA-N 0.000 description 1
- OYPRJOBELJOOCE-UHFFFAOYSA-N calcium Chemical compound [Ca] OYPRJOBELJOOCE-UHFFFAOYSA-N 0.000 description 1
- -1 lanthanum oxysulfide phosphor Chemical compound 0.000 description 1
- 239000000203 mixture Substances 0.000 description 1
- 229910052761 rare earth metal Inorganic materials 0.000 description 1
- 229910052706 scandium Inorganic materials 0.000 description 1
- CIOAGBVUUVVLOB-UHFFFAOYSA-N strontium Chemical compound [Sr] CIOAGBVUUVVLOB-UHFFFAOYSA-N 0.000 description 1
- 229910052727 yttrium Inorganic materials 0.000 description 1
- HCHKCACWOHOZIP-UHFFFAOYSA-N zinc Chemical compound [Zn] HCHKCACWOHOZIP-UHFFFAOYSA-N 0.000 description 1
- 229910052725 zinc Inorganic materials 0.000 description 1
Description
その他、下記一般式(10)で表される蛍光体、および下記一般式(11)で表される蛍光体も挙げられる。
(La1−x−y Eu x Lny)2O2S (10)
(一般式(10)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。)(一般式(10)で表される酸硫化ランタン蛍光体をLOS蛍光体と呼ぶ。)
(k−x)MgO・xAF2・GeO2:yMn4+ (11)
(一般式(11)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。)(一般式(11)で表されるジャーマネート蛍光体をMGOF蛍光体と呼ぶ。)
In addition, the fluorescent substance represented by following General formula (10) and the fluorescent substance represented by following General formula (11) are also mentioned.
(La 1-x- y E u x L n y) 2 O 2 S (10)
(In the general formula (10), x and y each represent a number satisfying 0.02 ≦ x ≦ 0.50 and 0 ≦ y ≦ 0.50, and Ln represents Y, Gd, Lu, Sc, Sm and Er At least one trivalent rare earth element is represented. (The lanthanum oxysulfide phosphor represented by the general formula (10) is referred to as LOS phosphor.)
(K−x) MgO · x AF 2 · GeO 2 : y Mn 4+ (11)
(In the general formula (11), k, x and y each represent a number satisfying 2.8 ≦ k ≦ 5, 0.1 ≦ x ≦ 0.7, and 0.005 ≦ y ≦ 0.015, A is calcium (Ca), strontium (Sr), barium (Ba), zinc (Zn), or a mixture thereof) (a germanate phosphor represented by the general formula (11)) and an MGOF phosphor Call.)
Claims (35)
少なくとも、発光要素として青色半導体発光素子を有し、
波長をλ(nm)とし、
当該発光要素から主たる放射方向に出射される光の分光分布をΦelm(λ)、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φSSL(λ)とし、
Φelm(λ)を有する光は下記条件I、条件II、条件IVの少なくともいずれかを満たさず、φSSL(λ)を有する光は下記条件I、条件II、条件IVのすべてを満たすことを特徴とする発光装置。
条件I:
対象とな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* n、b* n(ただしnは1から15の自然数)とし、
対象となる光の相関色温度T(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前記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* 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ΔCnが、
−4.00 ≦ ΔCn ≦ 8.00 (nは1から15の自然数)
である。
条件II:
下記式(3)で表される対象となる光における飽和度差の平均が、
である。
ただし、ΔCn=√{(a* n)2+(b* n)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
条件IV:
対象となる光による照明を数学的に仮定した場合の前記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θn(度)(ただしnは1から15の自然数)とし、
対象となる光の相関色温度T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前記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θnref(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|Δhn|が、
0.00 度 ≦ |Δhn| ≦ 12.50 度 (nは1から15の自然数)
である。
ただし、Δhn=θn−θnrefとする。 A light emitting device comprising a light emitting element and a control element, comprising:
At least, it has a blue semiconductor light emitting element as a light emitting element,
Let the wavelength be λ (nm),
The spectral distribution of light emitted from the light emitting element in the main radiation direction is 要素 elm (λ), and the spectral distribution of light emitted from the light emitting device in the main radiation direction is φ SSL (λ)
[Phi elm light having a (lambda) is the following condition I, conditions II, does not satisfy at least one of the conditions IV, phi SSL light having a (lambda) is the following condition I, conditions II, to satisfy all the conditions IV Characteristic light emitting device.
Condition I:
The CIE 1976 L * a * b * color space a * and b * values in the following 15 types of modified Munsell color charts from # 01 to # 15 when the illumination by the target light is mathematically assumed: a * N , b * n (where n is a natural number from 1 to 15),
CIE 1976 L * a * b * color of said 15 types of modified Munsell color charts when it is mathematically assumed that the illumination with the reference light selected according to the correlated color temperature T (K) of the object light Assuming that the a * value and the b * value in the space are a * nref and b * nref (where n is a natural number from 1 to 15), the saturation difference ΔC n is
−4.00 ≦ ΔC n ≦ 8.00 (n is a natural number of 1 to 15)
It is.
Condition II:
The average of the degree of saturation difference in the target light represented by the following formula (3) is
It is .
However, the ΔC n = √ {(a * n) 2 + (b * n) 2} -√ {(a * nref) 2 + (b * nref) 2}.
15 types of modified Munsell color charts # 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
Condition IV:
The hue angle in the CIE 1976 L * a * b * color space of the 15 types of the modified Munsell color chip when the illumination by the target light is mathematically assumed is θ n (degree) (where n is 1 to 15) Natural numbers),
The hue in the CIE 1976 L * a * b * color space of the above 15 types of modified Munsell color charts when it is mathematically assumed that the illumination with the reference light selected according to the correlated color temperature T of the target light Assuming that the angle is θ nref (degree) (where n is a natural number from 1 to 15), the absolute value of the hue angle difference | Δh n |
0.00 degree ≦ | Δh n | ≦ 12.50 degree (n is a natural number of 1 to 15)
It is.
However, it is set as ( DELTA) hn = (theta) n- ( theta ) nref .
少なくとも、発光要素として青色半導体発光素子を有し、 At least a blue semiconductor light emitting element as a light emitting element;
波長をλ(nm)とし、 Let the wavelength be λ (nm),
当該発光要素から主たる放射方向に出射される光の分光分布をΦ The spectral distribution of light emitted from the light emitting element in the main radiation direction is Φ elmelm (λ)、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(Λ), the spectral distribution of light emitted from the light emitting device in the main radiation direction SSLSSL (λ)とし、(Λ),
Φ Φ elmelm (λ)を有する光は下記条件I、条件II、条件IVのすべてを満たし、φThe light having (λ) satisfies all of the following conditions I, II and IV, and φ SSLSSL (λ)を有する光も下記条件I、条件II、条件IVのすべてを満たすことを特徴とする発光装置。A light emitting device characterized in that light having (λ) also satisfies all of the following conditions I, II and IV.
条件I:Condition I:
対象とな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 CIE 1976 L of the following 15 types of modified Munsell color charts of # 01 to # 15 when the illumination by the target light is mathematically assumed ** aa ** bb ** 色空間におけるaA in color space ** 値、bValue b ** 値をそれぞれaEach value a ** nn 、b, B ** nn (ただしnは1から15の自然数)とし、(Where n is a natural number of 1 to 15),
対象となる光の相関色温度T(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前記15種類の修正マンセル色票のCIE 1976 L CIE 1976 L of the above 15 modified Munsell color charts when it is assumed mathematically that the illumination with the reference light selected according to the correlated color temperature T (K) of the light of interest ** aa ** bb ** 色空間におけるaA in color space ** 値、bValue b ** 値をそれぞれaEach value a ** nrefnref 、b, B ** nrefnref (ただしnは1から15の自然数)とした場合に、飽和度差ΔC(Where n is a natural number of 1 to 15), the saturation difference ΔC nn が、But,
−4.00 ≦ ΔC −4.00 ≦ ΔC n n ≦ 8.00 (nは1から15の自然数)≦ 8.00 (n is a natural number of 1 to 15)
である。It is.
条件II:Condition II:
下記式(3)で表される対象となる光における飽和度差の平均が、 The average of the degree of saturation difference in the target light represented by the following formula (3) is
である。It is.
ただし、ΔC However, ΔC nn =√{(a= {{(A ** nn )) 22 +(b+ (B ** nn )) 22 }−√{(a} -√ {(a ** nrefnref )) 22 +(b+ (B ** nrefnref )) 22 }とする。} And
15種類の修正マンセル色票 15 types of modified Munsell color votes
#01 7.5 P 4 /10 # 01 7.5 P 4/10
#02 10 PB 4 /10 # 02 10 PB 4/10
#03 5 PB 4 /12 # 03 5 PB 4/12
#04 7.5 B 5 /10 # 04 7.5 B 5/10
#05 10 BG 6 / 8 # 05 10 BG 6/8
#06 2.5 BG 6 /10 # 06 2.5 BG 6/10
#07 2.5 G 6 /12 # 07 2.5 G 6/12
#08 7.5 GY 7 /10 # 08 7.5 GY 7/10
#09 2.5 GY 8 /10 # 09 2.5 GY 8/10
#10 5 Y 8.5/12 # 10 5 Y 8.5 / 12
#11 10 YR 7 /12 # 11 10 YR 7/12
#12 5 YR 7 /12 # 12 5 YR 7/12
#13 10 R 6 /12 # 13 10 R 6/12
#14 5 R 4 /14 # 14 5 R 4/14
#15 7.5 RP 4 /12 # 15 7.5 RP 4/12
条件IV:Condition IV:
対象となる光による照明を数学的に仮定した場合の前記15種類の修正マンセル色票のCIE 1976 L CIE 1976 L of the 15 modified Munsell color charts given mathematically assuming illumination by the light of interest ** aa ** bb ** 色空間における色相角をθThe hue angle θ in color space nn (度)(ただしnは1から15の自然数)とし、(Degree) (where n is a natural number from 1 to 15),
対象となる光の相関色温度T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前記15種類の修正マンセル色票のCIE 1976 L CIE 1976 L of the 15 modified Munsell color charts when mathematically assuming illumination with a reference light selected according to the correlated color temperature T of the light of interest ** aa ** bb ** 色空間における色相角をθThe hue angle θ in color space nrefnref (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(Degree) (where n is a natural number of 1 to 15), the absolute value of the hue angle difference | nn |が、But
0.00 度 ≦ |Δh 0.00 degree ≦ | Δ h nn | ≦ 12.50 度 (nは1から15の自然数)≦ 12.50 degrees (n is a natural number from 1 to 15)
である。It is.
ただし、Δh However, Δh nn =θ= Θ nn −θ−θ nrefnref とする。I assume.
Φ Φ elmelm (λ)を有する光は下記条件1を満たさず、φThe light having (λ) does not satisfy the following condition 1 and φ SSLSSL (λ)を有する光は下記条件1を満たすことを特徴とする発光装置。A light emitting device characterized in that light having (λ) satisfies condition 1 below.
条件1:Condition 1:
対象となる光の分光分布をφ(λ)、対象となる光の相関色温度Tに応じて選択される基準の光の分光分布をφ The spectral distribution of the light of interest is φ (λ), and the spectral distribution of reference light selected according to the correlated color temperature T of the light of interest is φ refref (λ)、(Λ),
対象となる光の三刺激値を(X、Y、Z)、 The tristimulus values of the target light (X, Y, Z),
前記相関色温度Tに応じて選択される基準の光の三刺激値を(X The tristimulus value of the reference light selected according to the correlated color temperature T (X refref 、Y, Y refref 、Z, Z refref )とし、)age,
対象となる光の規格化分光分布S(λ)と、対象となる光の基準の光の規格化分光分布S The normalized spectral distribution S (λ) of the target light and the normalized spectral distribution S of the reference light of the target light refref (λ)と、これら規格化分光分布の差ΔS(λ)をそれぞれ、(Λ) and the difference ΔS (λ) of these normalized spectral distributions are
S(λ)=φ(λ)/Y S (λ) = φ (λ) / Y
S S refref (λ)=φ(Λ) = φ refref (λ)/Y(Λ) / Y refref
ΔS(λ)=S ΔS (λ) = S refref (λ)−S(λ)(Λ) -S (λ)
と定義し、Defined as
波長380nm以上780nm以下の範囲で、前記S(λ)の最長波長極大値を与える波長をλ In the wavelength range of 380 nm to 780 nm, the wavelength giving the longest wavelength maximum value of S (λ) is λ RL−maxRL-max (nm)とした際に、前記λ(Λ) where λ RL−maxRL-max よりも長波長側にS(λS (λ RL−maxRL-max )/2となる波長Λ4が存在する場合においては、If there is a wavelength Λ4 of
下記数式(1)で表される指標A Index A represented by the following formula (1) cgcg が、But,
−10.0 < A -10.0 <A cgcg ≦ 120.0 ≦ 120.0
であり、And
一方、波長380nm以上780nm以下の範囲で、前記S(λ)の最長波長極大値を与える波長をλ On the other hand, in the wavelength range of 380 nm to 780 nm, the wavelength giving the longest wavelength maximum value of S (λ) is λ RL−maxRL-max (nm)とした際に、前記λ(Λ) where λ RL−maxRL-max よりも長波長側にS(λS (λ RL−maxRL-max )/2となる波長Λ4が存在しない場合においては、In the case where there is no wavelength Λ4 that is
下記数式(2)で表される指標A Index A represented by the following formula (2) cgcg が、But,
−10.0 < A -10.0 <A cgcg ≦ 120.0 ≦ 120.0
である。It is.
Φ Φ elmelm (λ)を有する光は下記条件1を満たし、φThe light having (λ) satisfies the following condition 1 and φ SSLSSL (λ)を有する光も下記条件1を満たすことを特徴とする発光装置。A light emitting device characterized in that the light having (λ) also satisfies the following condition 1.
条件1:Condition 1:
対象となる光の分光分布をφ(λ)、対象となる光の相関色温度Tに応じて選択される基準の光の分光分布をφ The spectral distribution of the light of interest is φ (λ), and the spectral distribution of reference light selected according to the correlated color temperature T of the light of interest is φ refref (λ)、(Λ),
対象となる光の三刺激値を(X、Y、Z)、 The tristimulus values of the target light (X, Y, Z),
前記相関色温度Tに応じて選択される基準の光の三刺激値を(X The tristimulus value of the reference light selected according to the correlated color temperature T (X refref 、Y, Y refref 、Z, Z refref )とし、)age,
対象となる光の規格化分光分布S(λ)と、対象となる光の基準の光の規格化分光分布S The normalized spectral distribution S (λ) of the target light and the normalized spectral distribution S of the reference light of the target light refref (λ)と、これら規格化分光分布の差ΔS(λ)をそれぞれ、(Λ) and the difference ΔS (λ) of these normalized spectral distributions are
S(λ)=φ(λ)/Y S (λ) = φ (λ) / Y
S S refref (λ)=φ(Λ) = φ refref (λ)/Y(Λ) / Y refref
ΔS(λ)=S ΔS (λ) = S refref (λ)−S(λ)(Λ) -S (λ)
と定義し、Defined as
波長380nm以上780nm以下の範囲で、前記S(λ)の最長波長極大値を与える波長をλ In the wavelength range of 380 nm to 780 nm, the wavelength giving the longest wavelength maximum value of S (λ) is λ RL−maxRL-max (nm)とした際に、前記λ(Λ) where λ RL−maxRL-max よりも長波長側にS(λS (λ RL−maxRL-max )/2となる波長Λ4が存在する場合においては、If there is a wavelength Λ4 of
下記数式(1)で表される指標A Index A represented by the following formula (1) cgcg が、But,
−10.0 < A -10.0 <A cgcg ≦ 120.0 ≦ 120.0
であり、And
一方、波長380nm以上780nm以下の範囲で、前記S(λ)の最長波長極大値を与える波長をλ On the other hand, in the wavelength range of 380 nm to 780 nm, the wavelength giving the longest wavelength maximum value of S (λ) is λ RL−maxRL-max (nm)とした際に、前記λ(Λ) where λ RL−maxRL-max よりも長波長側にS(λS (λ RL−maxRL-max )/2となる波長Λ4が存在しない場合においては、In the case where there is no wavelength Λ4 that is
下記数式(2)で表される指標A Index A represented by the following formula (2) cgcg が、But,
−10.0 < A -10.0 <A cgcg ≦ 120.0 ≦ 120.0
である。It is.
Φ Φ elmelm (λ)を有する光は下記条件2を満たさず、φThe light having (λ) does not satisfy the following condition 2 and φ SSLSSL (λ)を有する光は下記条件2を満たすことを特徴とする発光装置。A light emitting device characterized in that light having (λ) satisfies condition 2 below.
条件2:Condition 2:
対象となる光の分光分布φ(λ)は、ANSI C78.377で定義される黒体放射軌跡からの距離D The spectral distribution φ (λ) of the light of interest is the distance D from the black body radiation trajectory defined by ANSI C 78.377. uvuv が、But,
−0.0220 ≦ D −0.0220 ≦ D uvuv < 0 <0
である。It is.
Φ Φ elmelm (λ)を有する光は下記条件2を満たし、φThe light having (λ) satisfies the following condition 2 and φ SSLSSL (λ)を有する光も下記条件2を満たすことを特徴とする発光装置。A light emitting device characterized in that the light having (λ) also satisfies the following condition 2.
条件2:Condition 2:
対象となる光の分光分布φ(λ)は、ANSI C78.377で定義される黒体放射軌跡からの距離D The spectral distribution φ (λ) of the light of interest is the distance D from the black body radiation trajectory defined by ANSI C 78.377. uvuv が、But,
−0.0220 ≦ D −0.0220 ≦ D uvuv < 0 <0
である。It is.
Φ Φ elmelm (λ)を有する光は下記条件3を満たさず、φThe light having (λ) does not satisfy the following condition 3 and φ SSLSSL (λ)を有する光は下記条件3を満たすことを特徴とする発光装置。A light emitting device characterized in that light having (λ) satisfies condition 3 below.
条件3:Condition 3:
対象となる光の分光分布φ(λ)は、430nm以上495nm以下の範囲における分光強度の最大値をφ The spectral distribution φ (λ) of the light of interest is the maximum value of the spectral intensity in the range of 430 nm to 495 nm. BM−maxBM-max 、465nm以上525nm以下の範囲における分光強度の最小値をφ, The minimum value of the spectral intensity in the range of 465 nm or more and 525 nm or less BG−minBG-min と定義した際に、When you define
0.2250 ≦ φ 0.2250 φ φ BG−minBG-min /φ/ Φ BM−maxBM-max ≦ 0.7000 ≦ 0.7000
である。It is.
Φ Φ elmelm (λ)を有する光は下記条件3を満たし、φThe light having (λ) satisfies the following condition 3 and φ SSLSSL (λ)を有する光も下記条件3を満たすことを特徴とする発光装置。A light emitting device characterized in that the light having (λ) also satisfies the following condition 3.
条件3:Condition 3:
対象となる光の分光分布φ(λ)は、430nm以上495nm以下の範囲における分光強度の最大値をφ The spectral distribution φ (λ) of the light of interest is the maximum value of the spectral intensity in the range of 430 nm to 495 nm. BM−maxBM-max 、465nm以上525nm以下の範囲における分光強度の最小値をφ, The minimum value of the spectral intensity in the range of 465 nm or more and 525 nm or less BG−minBG-min と定義した際に、When you define
0.2250 ≦ φ 0.2250 φ φ BG−minBG-min /φ/ Φ BM−maxBM-max ≦ 0.7000 ≦ 0.7000
である。It is.
Φ Φ elmelm (λ)を有する光は下記条件4を満たさず、φThe light having (λ) does not satisfy the following condition 4 and φ SSLSSL (λ)を有する光は下記条件4を満たすことを特徴とする発光装置。A light emitting device characterized in that light having (λ) satisfies condition 4 below.
条件4:Condition 4:
対象となる光の分光分布φ(λ)は、590nm以上780nm以下の範囲における分光強度の最大値をφ The spectral distribution φ (λ) of the light of interest is the maximum value of the spectral intensity in the range of 590 nm to 780 nm. RM−maxRM-max と定義した際に、前記φWhen defined as RM−maxRM-max を与える波長λWavelength λ giving RM−maxRM-max が、But,
605(nm) ≦ λ 605 (nm) ≦ λ RM−maxRM-max ≦ 653(nm) ≦ 653 (nm)
である。It is.
Φ Φ elmelm (λ)を有する光は下記条件4を満たし、φThe light having (λ) satisfies the following condition 4 and φ SSLSSL (λ)を有する光も下記条件4を満たすことを特徴とする発光装置。A light emitting device characterized in that the light having (λ) also satisfies the following condition 4.
条件4:Condition 4:
対象となる光の分光分布φ(λ)は、590nm以上780nm以下の範囲における分光強度の最大値をφ The spectral distribution φ (λ) of the light of interest is the maximum value of the spectral intensity in the range of 590 nm to 780 nm. RM−maxRM-max と定義した際に、前記φWhen defined as RM−maxRM-max を与える波長λWavelength λ giving RM−maxRM-max が、But,
605(nm) ≦ λ 605 (nm) ≦ λ RM−maxRM-max ≦ 653(nm) ≦ 653 (nm)
である。It is.
Φ Φ elmelm (λ)を有する光は下記条件5を満たさず、φThe light having (λ) does not satisfy the following condition 5 and φ SSLSSL (λ)を有する光は下記条件5を満たすことを特徴とする発光装置。A light emitting device characterized in that light having (λ) satisfies condition 5 below.
条件5:Condition 5:
対象となる光の分光分布φ(λ)において、前記φ In the spectral distribution φ (λ) of the light of interest, BM−maxBM-max を与える波長λWavelength λ giving BM−maxBM-max が、But,
430(nm) ≦ λ 430 (nm) ≦ λ BM−maxBM-max ≦ 480(nm) ≦ 480 (nm)
である。It is.
Φ Φ elmelm (λ)を有する光は下記条件5を満たし、φThe light having (λ) satisfies the following condition 5 and φ SSLSSL (λ)を有する光も下記条件5を満たすことを特徴とする発光装置。A light emitting device characterized in that the light having (λ) also satisfies the following condition 5:
条件5:Condition 5:
対象となる光の分光分布φ(λ)において、前記φ In the spectral distribution φ (λ) of the light of interest, BM−maxBM-max を与える波長λWavelength λ giving BM−maxBM-max が、But,
430(nm) ≦ λ 430 (nm) ≦ λ BM−maxBM-max ≦ 480(nm) ≦ 480 (nm)
である。It is.
当該発光要素から主たる放射方向に出射される光の分光分布から導出される前記飽和度差の平均をSAT The average of the saturation differences derived from the spectral distribution of light emitted from the light emitting element in the main radiation direction is SAT aveave (Φ(Φ elmelm )、),
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から導出される前記飽和度差の平均をSAT The average of the saturation differences derived from the spectral distribution of light emitted from the light emitting device in the main radiation direction is SAT aveave (φ(Φ SSLSSL )と定義した場合に、When defined as)
SAT SAT aveave (Φ(Φ elmelm )<SAT) <SAT aveave (φ(Φ SSLSSL ))
を満たすことを特徴とする発光装置。A light emitting device characterized in that
当該発光要素から主たる放射方向に出射される光の分光分布から導出されるD D derived from the spectral distribution of light emitted from the light emitting element in the main radiation direction uvuv をDD uvuv (Φ(Φ elmelm )、),
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から導出されるD D derived from the spectral distribution of light emitted from the light emitting device in the main radiation direction uvuv をDD uvuv (φ(Φ SSLSSL )と定義した場合に、When defined as)
D D uvuv (φ(Φ SSLSSL )<D) <D uvuv (Φ(Φ elmelm ))
を満たすことを特徴とする発光装置。A light emitting device characterized in that
当該発光要素から主たる放射方向に出射される光の分光分布から導出されるA A derived from the spectral distribution of light emitted from the light emitting element in the main radiation direction cgcg をAA cgcg (Φ(Φ elmelm )、),
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から導出されるA A derived from the spectral distribution of light emitted from the light emitting device in the main radiation direction cgcg をAA cgcg (φ(Φ SSLSSL )と定義した場合に、When defined as)
A A cgcg (φ(Φ SSLSSL )<A) <A cgcg (Φ(Φ elmelm ))
を満たすことを特徴とする発光装置。A light emitting device characterized in that
当該制御要素は380nm≦λ(nm)≦780nmの光を吸収または反射する光学フィルターであることを特徴とする発光装置。 A light-emitting device characterized in that the control element is an optical filter that absorbs or reflects light of 380 nm ≦ λ (nm) ≦ 780 nm.
当該制御要素が発光要素から出射される光の集光および/または拡散機能を兼ね備えていることを特徴とする発光装置。 A light emitting device characterized in that the control element also has a function of condensing and / or diffusing light emitted from the light emitting element.
当該制御要素の集光および/または拡散機能が凹レンズ、凸レンズ、フレネルレンズの少なくとも1つの機能によって実現することを特徴とする発光装置。 A light-emitting device, 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.
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5lx以上10000lx以下であることを特徴とする発光装置。 The light emitted from the light emitting device in the radiation direction illuminates an object at an illuminance of 5 lx or more and 10000 lx or less.
Φ Φ elmelm (λ)を有する光は下記条件6を満たさず、φThe light having (λ) does not satisfy the following condition 6 and φ SSLSSL (λ)を有する光は下記条件6を満たすことを特徴とする発光装置。A light emitting device characterized in that light having (λ) satisfies condition 6 below.
条件6:Condition 6:
対象となる光の分光分布φ(λ)は The spectral distribution φ (λ) of the light of interest is
0.1800 ≦ φ 0.1800 φ φ BG−minBG-min /φ/ Φ RM−maxRM-max ≦ 0.8500 ≦ 0.8500
である。It is.
Φ Φ elmelm (λ)を有する光は下記条件7を満たさず、φThe light having (λ) does not satisfy the following condition 7 and φ SSLSSL (λ)を有する光は下記条件7を満たすことを特徴とする発光装置。A light emitting device characterized in that light having (λ) satisfies condition 7 below.
条件7:Condition 7:
対象となる光の分光分布φ(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 The radiation efficiency K (lm / W) in the wavelength range of 380 nm or more and 780 nm or less derived from the spectral distribution φ (λ) of the target light
210.0 lm/W ≦ K ≦ 290.0 lm/W 210.0 lm / W ≦ K ≦ 290.0 lm / W
である。It is.
Φ Φ elmelm (λ)を有する光は下記条件8を満たさず、φThe light having (λ) does not satisfy the following condition 8 and φ SSLSSL (λ)を有する光は下記条件8を満たすことを特徴とする発光装置。A light having (λ) satisfies the following condition 8;
条件8:Condition 8:
対象となる光の相関色温度T(K)が The correlated color temperature T (K) of the light of interest
2600 K ≦ T ≦ 7700 K 2600 K ≦ T ≦ 7700 K
である。It is.
Φ Φ elmelm (λ)を有する光は下記条件5、条件7、及び条件8の少なくとも1つを満たし、φThe light having (λ) satisfies at least one of the following condition 5, condition 7, and condition 8, and φ SSLSSL (λ)を有する光は下記条件5、条件7、及び条件8のうち前記ΦThe light having (λ) has the above Φ among conditions 5, 7 and 8 below. elmelm (λ)を有する光が満たさない条件があれば、そのうち少なくとも1つを満たすことを特徴とする発光装置。What is claimed is: 1. A light emitting device characterized by satisfying at least one of the conditions under which light having (λ) is not satisfied.
条件5:Condition 5:
対象となる光の分光分布φ(λ)において、前記φ In the spectral distribution φ (λ) of the light of interest, BM−maxBM-max を与える波長λWavelength λ giving BM−maxBM-max が、But,
430(nm) ≦ λ 430 (nm) ≦ λ BM−maxBM-max ≦ 480(nm) ≦ 480 (nm)
である。It is.
条件7:Condition 7:
対象となる光の分光分布φ(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 The radiation efficiency K (lm / W) in the wavelength range of 380 nm or more and 780 nm or less derived from the spectral distribution φ (λ) of the target light
210.0 lm/W ≦ K ≦ 290.0 lm/W 210.0 lm / W ≦ K ≦ 290.0 lm / W
である。It is.
条件8:Condition 8:
対象となる光の相関色温度T(K)が The correlated color temperature T (K) of the light of interest
2600 K ≦ T ≦ 7700 K 2600 K ≦ T ≦ 7700 K
である。It is.
Φ Φ elmelm (λ)を有する光は下記条件5、条件6、及び条件8の少なくとも1つを満たし、φThe light having (λ) satisfies at least one of the following condition 5, condition 6, and condition 8, and φ SSLSSL (λ)を有する光は下記条件5、条件6、及び条件8のうち前記ΦThe light having (λ) has the above-mentioned の う ち among the following condition 5, condition 6, and condition 8 elmelm (λ)を有する光が満たさない条件があれば、そのうち少なくとも1つを満たすことを特徴とする発光装置。What is claimed is: 1. A light emitting device characterized by satisfying at least one of the conditions under which light having (λ) is not satisfied.
条件5:Condition 5:
対象となる光の分光分布φ(λ)において、前記φ In the spectral distribution φ (λ) of the light of interest, BM−maxBM-max を与える波長λWavelength λ giving BM−maxBM-max が、But,
430(nm) ≦ λ 430 (nm) ≦ λ BM−maxBM-max ≦ 480(nm) ≦ 480 (nm)
である。It is.
条件6:Condition 6:
対象となる光の分光分布φ(λ)は The spectral distribution φ (λ) of the light of interest is
0.1800 ≦ φ 0.1800 φ φ BG−minBG-min /φ/ Φ RM−maxRM-max ≦ 0.8500 ≦ 0.8500
である。It is.
条件8:Condition 8:
対象となる光の相関色温度T(K)が The correlated color temperature T (K) of the light of interest
2600 K ≦ T ≦ 7700 K 2600 K ≦ T ≦ 7700 K
である。It is.
Φ Φ elmelm (λ)を有する光は下記条件5〜条件7の少なくとも1つを満たし、φThe light having (λ) satisfies at least one of the following conditions 5 to 7, and φ SSLSSL (λ)を有する光は下記条件5〜条件7のうち前記ΦThe light having (λ) has the above Φ among conditions 5 to 7 below. elmelm (λ)を有する光が満たさない条件があれば、そのうち少なくとも1つを満たすことを特徴とする発光装置。What is claimed is: 1. A light emitting device characterized by satisfying at least one of the conditions under which light having (λ) is not satisfied.
条件5:Condition 5:
対象となる光の分光分布φ(λ)において、前記φ In the spectral distribution φ (λ) of the light of interest, BM−maxBM-max を与える波長λWavelength λ giving BM−maxBM-max が、But,
430(nm) ≦ λ 430 (nm) ≦ λ BM−maxBM-max ≦ 480(nm) ≦ 480 (nm)
である。It is.
条件6:Condition 6:
対象となる光の分光分布φ(λ)は The spectral distribution φ (λ) of the light of interest is
0.1800 ≦ φ 0.1800 φ φ BG−minBG-min /φ/ Φ RM−maxRM-max ≦ 0.8500 ≦ 0.8500
である。It is.
条件7:Condition 7:
対象となる光の分光分布φ(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 The radiation efficiency K (lm / W) in the wavelength range of 380 nm or more and 780 nm or less derived from the spectral distribution φ (λ) of the target light
210.0 lm/W ≦ K ≦ 290.0 lm/W 210.0 lm / W ≦ K ≦ 290.0 lm / W
である。It is.
Φ Φ elmelm (λ)を有する光は下記条件5〜条件8の全てを満たし、かつ、φThe light having (λ) satisfies all of the following conditions 5 to 8 and φ SSLSSL (λ)を有する光も下記条件5〜条件8の全てを満たすことを特徴とする発光装置。A light emitting device characterized in that light having (λ) also satisfies all of the following conditions 5 to 8:
条件5:Condition 5:
対象となる光の分光分布φ(λ)において、前記φ In the spectral distribution φ (λ) of the light of interest, BM−maxBM-max を与える波長λWavelength λ giving BM−maxBM-max が、But,
430(nm) ≦ λ 430 (nm) ≦ λ BM−maxBM-max ≦ 480(nm) ≦ 480 (nm)
である。It is.
条件6:Condition 6:
対象となる光の分光分布φ(λ)は The spectral distribution φ (λ) of the light of interest is
0.1800 ≦ φ 0.1800 φ φ BG−minBG-min /φ/ Φ RM−maxRM-max ≦ 0.8500 ≦ 0.8500
である。It is.
条件7:Condition 7:
対象となる光の分光分布φ(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 The radiation efficiency K (lm / W) in the wavelength range of 380 nm or more and 780 nm or less derived from the spectral distribution φ (λ) of the target light
210.0 lm/W ≦ K ≦ 290.0 lm/W 210.0 lm / W ≦ K ≦ 290.0 lm / W
である。It is.
条件8:Condition 8:
対象となる光の相関色温度T(K)が The correlated color temperature T (K) of the light of interest
2600 K ≦ T ≦ 7700 K 2600 K ≦ T ≦ 7700 K
である。It is.
前記発光要素として、さらに緑色蛍光体を有することを特徴とする発光装置。 A light emitting device further comprising a green phosphor as the light emitting element.
前記発光要素として、さらに赤色蛍光体を有することを特徴とする発光装置。 A light emitting device further comprising a red phosphor as the light emitting element.
前記緑色蛍光体は、前記緑色蛍光体単体の光励起時の発光強度最大値を与える波長λ The green phosphor has a wavelength λ giving a maximum emission intensity at the time of light excitation of the green phosphor alone. PHOS−GM−maxPHOS-GM-max が511nm以上543nm以下であり、Is at least 511 nm and at most 543 nm,
その半値全幅W The full width half maximum W PHOS−GM−fwhmPHOS-GM-fwhm が90nm以上110nm以下であることを特徴とする発光装置。Is 90 nm or more and 110 nm or less.
前記赤色蛍光体は、前記赤色蛍光体単体の光励起時の発光強度最大値を与える波長λ The red phosphor has a wavelength λ that gives the maximum emission intensity at the time of light excitation of the red phosphor alone. PHOS−RM−maxPHOS-RM-max が622nm以上663nm以下であり、Is 622 nm or more and 663 nm or less,
その半値全幅W The full width half maximum W PHOS−RM−fwhmPHOS-RM-fwhm が80nm以上105nm以下であることを特徴とする発光装置。Is 80 nm or more and 105 nm or less.
前記緑色蛍光体は、Ca The green phosphor is Ca 33 (Sc,Mg)(Sc, Mg) 22 SiSi 33 OO 1212 :Ce(CSMS蛍光体)、CaSc: Ce (CSMS phosphor), CaSc 22 OO 44 :Ce(CSO蛍光体)、Lu: Ce (CSO phosphor), Lu 33 AlAl 55 OO 1212 :Ce(LuAG蛍光体)、またはY: Ce (LuAG phosphor) or Y 33 (Al,Ga)(Al, Ga) 55 OO 1212 :Ce(G−YAG蛍光体)であることを特徴とする発光装置。: A light emitting device characterized by being Ce (G-YAG phosphor).
前記赤色蛍光体は(Sr,Ca)AlSiN The red phosphor is (Sr, Ca) AlSiN 33 :Eu(SCASN蛍光体)、(CaAlSiN: Eu (SCASN phosphor), (CaAlSiN 33 )) 1−x1-x (Si(Si 22 NN 22 O)O) xx :Eu(ただし、xは0<x<0.5)(CASON蛍光体)、またはCaAlSiN: Eu (where x is 0 <x <0.5) (CASON phosphor) or CaAlSiN 33 :Eu(CASN蛍光体)を含むことを特徴とする発光装置。: A light emitting device including Eu (CASN phosphor).
前記青色半導体発光素子は、前記青色半導体発光素子単体のパルス駆動時のドミナント波長λ The blue semiconductor light emitting device has a dominant wavelength λ during pulse driving of the single blue semiconductor light emitting device. CHIP−BM−domCHIP-BM-dom が452.5nm以上470nm以下であるAlInGaN系発光素子であり、An AlInGaN-based light emitting device having a wavelength of 452.5 nm to 470 nm,
前記緑色蛍光体は、前記緑色蛍光体単体の光励起時の発光強度最大値を与える波長λ The green phosphor has a wavelength λ giving a maximum emission intensity at the time of light excitation of the green phosphor alone. PHOS−GM−maxPHOS-GM-max が515nm以上535nm以下で、その半値全幅WIs 515 nm to 535 nm, and its full width at half maximum W PHOS−GM−fwhmPHOS-GM-fwhm が90nm以上110nm以下であることを特徴とする、CaScIs from 90 nm to 110 nm, CaSc 22 OO 44 :Ce(CSO蛍光体)またはLu: Ce (CSO phosphor) or Lu 33 AlAl 55 OO 1212 :Ce(LuAG蛍光体)であり、: Ce (LuAG phosphor),
前記赤色蛍光体は、前記赤色蛍光体単体の光励起時の発光強度最大値λ The red phosphor has a light emission intensity maximum value λ at the time of light excitation of the red phosphor alone. PHOS−RM−maxPHOS-RM-max を与える波長が640nm以上663nm以下で、その半値全幅WTo give a wavelength of 640 nm or more and 663 nm or less, and its full width at half maximum W PHOS−RM−fwhmPHOS-RM-fwhm が80nm以上105nm以下であることを特徴とする、(CaAlSiNIs not less than 80 nm and not more than 105 nm, (CaAlSiN 33 )) 1−x1-x (Si(Si 22 NN 22 O)O) xx :Eu(ただし、xは0<x<0.5)(CASON蛍光体)またはCaAlSiN: Eu (where x is 0 <x <0.5) (CASON phosphor) or CaAlSiN 33 :Eu(CASN蛍光体)である: Eu (CASN phosphor)
ことを特徴とする発光装置。A light emitting device characterized by
前記緑色蛍光体は、狭帯域緑色蛍光体であることを特徴とする発光装置。 The light emitting device, wherein the green phosphor is a narrow band green phosphor.
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