TW200303416A - Optical measurement device - Google Patents

Optical measurement device Download PDF

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TW200303416A
TW200303416A TW91135055A TW91135055A TW200303416A TW 200303416 A TW200303416 A TW 200303416A TW 91135055 A TW91135055 A TW 91135055A TW 91135055 A TW91135055 A TW 91135055A TW 200303416 A TW200303416 A TW 200303416A
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incident
light
optical
measurement
incident surface
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TW91135055A
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TW580569B (en
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Hiroaki Iio
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Minolta Co Ltd
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Abstract

The object is to provide an optical measurement device for increasing the precision of the measured value of the sensed light quantity from the emitted surface by inhibiting the non-uniformity of the emitted light quantity from plural emitted surfaces even under the situation that the optical distribution characteristic of the object to be measured is asymmetric. To achieve the object, the optical measurement device comprises the fiber bundle 22 on the plural emitted surfaces to split the light incident into the incident surface A from the measured object. The structure of incident surface A is divided into plural incident regions A11~A32, and each emitted surface emits light onto plural different incident regions A11~A32 which are not adjacent.

Description

200303416 五、發明說明(1) 【發明所屬之技術領域】 本發明係有關於包括具有將射入入射面之來自被量測 物之光分岐後射出之複數射出面之光分岐裝置之量測用光 學裝置。本發明例如應用於用以量測或調整液晶面板等之 顯示特性(色度、亮度、色差等)之三刺激值型光電色度 計。 【先前技術】 參照表示本發明之一實施例之圖3說明在以往之量測 用光學裝置。 在圖3,光學裝置由物鏡21、束光纖22以及光電轉換 部2 3構成。 物鏡2 1配置成和被量測物Q之被量測區域AR相向’將 自被量測區域AR出來之光束聚光後導向束光纖2 2之入射面 A。束光纖2 2由多條光纖素線成束而成,具有一個入射面A 及3個射出面B1、B2、B3。射入入射面A之光束分支成3條 光束後自3個射出面Bl、B2、B3射出。束光纖22配置成入 射面A位於距離物鏡21之像側主點和其焦距f大致相等之距 離之位置。藉著這種配置,自被量測區域出來之光之中 只有射出^ α以下之光束射入入射面A。依據物鏡2 1之焦 距f和束光纖22之直徑D決定射出角α之大小。一般射出角 α設為約2 · 5度以下。 光電轉換部23由各自和3個射出面Bl、Β2、Β3對應的 配置之3個光譜靈敏度補償濾光器231a、231b、231c及3個 感光感測器232a、2 32b、232c構成。感光感測器2 3 2a〜c利200303416 V. Description of the invention (1) [Technical field to which the invention belongs] The present invention relates to a measurement device including a light divergence device including a plurality of light exit surfaces having a light exit from a measured object that is incident on an incident surface and divided. Optical device. The present invention is applied to, for example, a tristimulus value type photoelectric colorimeter for measuring or adjusting display characteristics (chroma, brightness, color difference, etc.) of a liquid crystal panel or the like. [Prior Art] A conventional optical device for measurement is described with reference to FIG. 3 showing an embodiment of the present invention. In Fig. 3, the optical device includes an objective lens 21, a beam fiber 22, and a photoelectric conversion section 23. The objective lens 21 is arranged so as to be opposed to the measurement area AR of the measurement object Q, and converges the light beam from the measurement area AR to the incident surface A of the optical fiber 22. The bundle optical fiber 22 is formed by bundling a plurality of optical fiber prime wires, and has one incident surface A and three exit surfaces B1, B2, and B3. The light beam incident on the incident surface A is branched into three light beams and then emitted from the three exit surfaces Bl, B2, and B3. The bundle optical fiber 22 is arranged such that the incident surface A is located at a distance substantially equal to the focal point f of the image side of the objective lens 21 and its focal length f. With this configuration, only the light beams that are less than ^ α out of the light emitted from the measurement area enter the incident surface A. The magnitude of the exit angle α is determined based on the focal length f of the objective lens 21 and the diameter D of the beam fiber 22. Generally, the emission angle α is set to about 2.5 degrees or less. The photoelectric conversion unit 23 is composed of three spectral sensitivity compensation filters 231a, 231b, 231c, and three photosensitive sensors 232a, 232b, and 232c, which are arranged corresponding to the three emission surfaces Bl, B2, and B3, respectively. Photo sensor 2 3 2a ~ c

2201-5287-Pf(Nl).ptd 第4頁 200303416 五、發明說明(2) 用光譜靈敏度補償濾光器23 la〜c具有接近色匹配函數之光 譜靈敏度,各自接受自射出面B1〜B3射出之光束。因而, 自光電轉換部23輸出將射入入射面A之光束分解成三原色 之色成分之電氣信號。依照該電氣信號計算被量測物Q之 三刺激值。 如圖1 1所示,在以往,將束光纖2 2之入射面A劃分成 中心角為1 2 0度而面積彼此相等之3個扇形之入射區域A j 1 、A j 2、A j 3。射入入射區域A j 1之光束被導向射出面B 1後 射出,射入入射區域A j2之光束被導向射出面B2後射出, 射入入射區域A j3之光束被導向射出面B3後射出。 【發明内容】 發明要解決之課題 在以往’因束光纖22之入射面A只劃分成3個入射區域 Ajl〜3,依據被量測物Q之配光特性,在3個入射區域Aji〜3 之間發生感光量之不勻(照度變動)。因而,在入射面A之 轉動角度位置相對於被量測物q之關係變化之情況,感光 感測裔2 3 2 a〜c之感光量變動,結果,有在量測值上所得到 之三刺激值變化之問題。 即,例如如圖6所不,考慮自被量測區域AR之某點射 入入射面A之截面為圓形之光束KSa。該光束KSa之中之上 半部之光束(圖6之以斜線表示之部分)射入入射面A之上 部,下半部之光束(圖6之無斜線之部分)射入入射面a 半部。這在被量職k配光特性相對於其法線係對稱之 情況無問題’但是在配光特性係非對稱之情況有問題。2201-5287-Pf (Nl) .ptd Page 4 200303416 V. Description of the invention (2) The spectral sensitivity compensation filter 23 la ~ c has a spectral sensitivity close to the color matching function, and each accepts self-emission surfaces B1 ~ B3 Of the beam. Therefore, an electrical signal is output from the photoelectric conversion section 23 to decompose the light beam incident on the incident surface A into color components of the three primary colors. According to the electrical signal, the three stimulus values of the measured object Q are calculated. As shown in FIG. 11, in the past, the incident surface A of the bundle optical fiber 2 was divided into three fan-shaped incident areas A j 1, A j 2, and A j 3 with a center angle of 120 degrees and an area equal to each other. . The light beam incident on the incident area A j 1 is directed toward the exit surface B 1 and emitted, and the light beam incident on the incident area A j 2 is directed on the exit surface B 2 and emitted, and the light beam incident on the incident area A j 3 is directed on the exit surface B 3 and emitted. [Summary of the Invention] The problem to be solved by the invention in the past was' the incident surface A of the bundle optical fiber 22 was divided into only three incident areas Ajl ~ 3, and according to the light distribution characteristics of the measured object Q, the incident areas Aji ~ 3 Variations in light sensitivity (illuminance variations) occur between them. Therefore, when the relationship between the rotational angle position of the incident surface A and the measured object q is changed, the photosensitive quantity of the photosensitive sensors 2 3 2 a to c varies. As a result, there are three obtained from the measured value. Problems with stimulus changes. That is, as shown in FIG. 6, for example, a light beam KSa having a circular cross section that is incident on the incident surface A from a point in the measurement area AR is considered. The upper half of the light beam KSa (the part indicated by the oblique line in FIG. 6) enters the upper part of the incident surface A, and the lower half of the light beam (the part without the oblique line in FIG. 6) enters the half of the incident surface a . This is not a problem when the measured light distribution characteristics are symmetrical with respect to its normal system ', but there are problems when the light distribution characteristics are asymmetric.

2201-5287-Pf(Nl).ptd f 5頁 200303416 五、發明說明(3) 即,如圖7所示,在自被量測物Q出來之光束KS之中向 上方出來之光束比向下方出來之光束大之情況,入射面A 之上半部變亮,下半部變暗。結果’在射入3個入射區域 A jl〜3之光量發生不勻。因此’在入射面A之轉動角度位置 相對於被量測物Q之關係變化之情況,對於同一感光感測 器232a〜c之感光量變動。 例如,在圖1 1所示之轉動角度位置之情況,上方之入 射區域A jl之感光量最多,但是束光纖22轉動而轉動角度 位置變化1 8 0度,入射區域A j 1來到下方時,其感光量變成 最少。 於是,在以往’依據被量測物Q和光學裝置之配置關 係在量測值上所得到之三刺激值就變化,有出現量測誤差 之問題。因在液晶面板之情況常看到配光特性在上下非對 稱之現象’在量測液晶顯示器之光學特性時成為問題。 本發明鐘於上述之問題點’其目的在於提供一種量測 用光學裝置,係被量測物之配光特性非對稱之情況,也儘 里抑制自複數射出面射出之光量之不勻,令依照來自射出 面之感光量所量測之量測值之精度提高。 解決課題之手段 本發明之量測用光學裝置,包括··具有將射入入射面 之來自被量測物之光分岐後射出之複數射出面之光分岐裝 置,在構造上將該入射面劃分成複數入射=自之 該射出面射出射入不相鄰之彼此相異之複數入射區域。 最好该量測用光學裝置包括將來自被量測物之光聚光2201-5287-Pf (Nl) .ptd f Page 2003200316 V. Explanation of the invention (3) That is, as shown in FIG. 7, among the light beams KS from the object Q to be measured, the light beams that are directed upwards are downward. When the outgoing beam is large, the upper half of the incident surface A becomes brighter and the lower half becomes darker. As a result, the amount of light incident on the three incident areas A jl to 3 is uneven. Therefore, when the relationship between the position of the rotation angle of the incident surface A and the object Q to be measured changes, the sensitivity of the same photosensitive sensors 232a to c varies. For example, in the case of the rotation angle position shown in FIG. 11, the light intensity of the incident area A jl above is the most, but the rotation angle position of the beam fiber 22 is changed by 180 degrees, and the incident area A j 1 comes to the bottom. , Its light sensitivity becomes the smallest. Therefore, in the past, the three stimulus values obtained from the measured values according to the configuration of the object to be measured Q and the optical device changed, and there was a problem of measurement errors. In the case of a liquid crystal panel, it is often seen that the light distribution characteristics are asymmetrical up and down ', which becomes a problem when measuring the optical characteristics of a liquid crystal display. The object of the present invention is to provide an optical device for measurement, which aims to provide an optical device for measurement, which is a case where the light distribution characteristics of the object to be measured are asymmetrical. The accuracy of the measurement value measured in accordance with the amount of light from the emitting surface is improved. Means for Solving the Problem The optical device for measurement of the present invention includes a light diverging device having a plurality of exit surfaces that diverge light from the object to be measured that is incident on the incident surface, and divides the incident surface structurally. Plurality of incidents = From this exit plane, the incidents are not incident on the multiple incident areas that are different from each other. Preferably, the measuring optical device includes condensing light from the object to be measured

2201-5287-Pf(Nl).ptd 第6頁 200303416 五、發明說明(4) 〜 "' "一""' ^裝置’將該光分岐裝置配置成該入射面位於距離該 水光裝置之像側主點和其焦距大致相等之距離之位置。 、^者’該量剛用光學裝置包括··第一聚光裝置,將來 自被量測物之光聚光;光圈止鐵,配置於該第一聚光裝置 之後f ;以及第二聚光裝置,將通過了該光圈止鐵之光聚 光’該光分岐裝置配置於相對於該第二聚光裝置該入射面 和該光圈止鐵變成共辆之關係之位置。 又’各自和各自之該射出面對應之複數入射區域位於 彼此相對於在該入射面之中心點對稱之位置。或者,各自 矛各自之°亥射出面對應之複數入射區域在該入射面位於隨 機之位置。 ^在構&上包括:感光裝置,和該光分岐裝置之各 出面相向的配置’將射入該入射面之光分解成色成 刀後轉換為電氣信赛·男斗々々 出之帝^ γ 4 #虎,计异1置,依照自該感光裝置輪 包軋仏唬计异三刺激值。 4 可應用於色度計等各種光學機器或量測機器。 = : = 型㈡以況,… -射面之來Μ皮量測物之= = = = ^ =射 將该入射面劃分成複數入射區域,自“ ’ '入不相鄰之彼此相異之複數入射區⑨;感面射出 和忒光分岐裝置之各自之射出面相向的配置之:有 ’將射入該入射面之光分解成三原色之色】,感光部 氣信號;以及計算裝置,依照自該感光裝置輪f轉換為電 •屯之電氣信 第7頁 2201 -5287-Pf(N 1). ptd 2003034162201-5287-Pf (Nl) .ptd Page 6 200303416 V. Description of the Invention (4) ~ " '" a " "' ^ device 'Configure the optical divergence device such that the incident surface is located away from the water The position of the image-side principal point of the optical device and a distance at which the focal length is approximately equal.者 者 'The optical device used for this quantity includes a first condensing device that condenses light from the object to be measured; an aperture stop is disposed behind the first condensing device f; and a second condensing device The device condenses the light passing through the aperture stop iron. The optical divergence device is arranged at a position where the entrance surface of the second condenser device and the aperture stop iron are in a common vehicle relationship. Also, each of the plural incident areas corresponding to the respective exit surfaces is located at positions symmetrical to each other with respect to the center point of the incident surface. Alternatively, the plurality of incident areas corresponding to the respective ° exit surfaces of the respective spears are located at random positions on the incident surfaces. ^ The structure & includes: a light-sensitive device, and a configuration facing each of the light diverging devices. The light incident on the incident surface is decomposed into a knife and converted into an electric letter. 4 # 虎 , 计 异 1 Set, according to the stimulus value of the different tristimulus from the photosensitive device. 4 It can be applied to various optical devices or measuring devices such as colorimeters. =: = Type, according to the situation, ...-The measurement surface of the measurement surface is = = = = ^ = The projection surface is divided into a plurality of incident areas, which are different from each other. A plurality of incident areas ⑨; the respective emitting surfaces of the sensing surface emitting and the chirping light divergence device are opposite to each other: there is' decompose the light incident on the incident surface into three primary colors], the gas signal of the photosensitive part; Converted from this photoreceptor wheel f to electricity • Tunzhi Electric Page 2201 -5287-Pf (N 1). Ptd 200303416

2201-5287-Pf(Nl).ptd 第8頁 200303416 五、發明說明(6) 算國際照明委員會(C I E )所制定之三刺激值(X、γ、z )、 xy Y (色度座標、亮度)、τ ΔυνΥ (相關色溫、來自黑體軌跡 之色差、亮度)等。 在圖2及圖3,量測頭2由包括物鏡21及束光纖22之量 測用光學糸Κ Κ 1和由光電轉換部2 3及放大部2 4構成之感光 系JK1構成。 光電轉換部2 3包括由3個光譜靈敏度補償濾光器2 3 1 a〜 c及S P C等構成之3感光感測器2 3 2 a〜c感光感測器2 3 2 a〜c各2201-5287-Pf (Nl) .ptd Page 8 200303416 V. Description of the invention (6) Calculate the three stimulus values (X, γ, z), xy Y (chromaticity coordinates, brightness, etc.) formulated by the International Commission for Illumination (CIE) ), Τ ΔυνΥ (correlated color temperature, color difference from blackbody locus, brightness), etc. In Figs. 2 and 3, the measuring head 2 is composed of an optical lens KK 1 for measurement including an objective lens 21 and a beam optical fiber 22, and a photosensitive system JK1 composed of a photoelectric conversion section 23 and an amplification section 24. The photoelectric conversion unit 2 3 includes 3 photo-sensing sensors 2 3 1 a to c and S P C, etc., which are each composed of 3 spectral sensitivity compensation filters 2 3 2 a to c.

自配置於係射出面B1、B 2、B 3之中心軸上,且良好的接收 自射出面Bl、B2、B3射出之光束之位置。光譜靈敏度補償 濾光器23 la〜c各自配置於感光感測器2 3 2 a〜c和射出面B1、 B2、B3之間之適當之位置。 光譜靈敏度補償濾光器2 3 1 a例如具有在紅光(r )之波 長區域具有靈敏度之濾光器特性。利用該濾光器特性將感 光感測器2 3 2 a補償成在紅光之波長區域具有大的靈敏度之 色匹配函數(X · bar ·又)之感光靈敏度。又,其他之光譜 A敏度補償濾光器231b及231c各自具有在綠光(G)或藍光 (B)之波長區域具有靈敏度之濾光器特性,利用該濾光器 特性將感光感測器2 32b補償成在綠光之波長區域具有大的It is arranged on the central axis of the emitting surfaces B1, B2, and B3, and receives the light beams emitted from the emitting surfaces B1, B2, and B3. The spectral sensitivity compensation filters 23 la to c are respectively disposed at appropriate positions between the photoreceptors 2 3 2 a to c and the emission surfaces B1, B2, and B3. The spectral sensitivity compensation filter 2 3 1 a has, for example, a filter characteristic having sensitivity in a wavelength region of red light (r). Using this filter characteristic, the photo sensor 2 3 2 a is compensated to the photosensitivity of a color matching function (X · bar · again) having a large sensitivity in the wavelength region of red light. In addition, the other spectral A sensitivity compensation filters 231b and 231c each have a filter characteristic having sensitivity in a wavelength region of green (G) or blue (B) light, and the photosensitive sensor is used to utilize the filter characteristic 2 32b is compensated to have a large

”色匹配函數(Y .bar · λ)之感*靈敏度,將感光 感測M32c補償成在Μ光之波長區域具有大的靈敏度之色 =配函i:(Z · bar · λ )之感光靈敏度。因此,自感光感測 器2=a〜c輸出相t於三刺激值(γ、γ、ζ)之電氣信號(感光 化號)。”Color matching function (Y .bar · λ), the sensitivity * sensitivity, compensates the light sensing M32c to a color with a large sensitivity in the wavelength region of M light = distribution i: (Z · bar · λ) Therefore, the electric signals (photosensitivity numbers) of phase t relative to the three stimulus values (γ, γ, ζ) are output from the photosensitive sensors 2 = a ~ c.

200303416 五、發明說明(7) 放大部2 4將自光電轉換部2 3所輸出之電氣信號放大至 既定之位準。 在圖3,束光纖2 2在軸向之中間部分分成3條,射入入 射面A之光束分開的向3個射出面Bl 、B2、B3射出。 如圖4所示,束光纖2 2之入射面A劃分成中心角6 0度且 面積彼此相等之6個扇形之入射區域A11、A1 2、A 2 1、A 2 2 、A 3 1、A 3 2。由圖4得知,入射區域A11和A1 2、入射區域 A 2 1和A 2 2、入射區域A 3 1和A 3 2各自位於以光軸l為中心之 點對稱之位置。射入這些位於點對稱之位置之2個入射區 域之光束自同一射出面射出。即,射入入射區域A i 1和A1 2 之光束被導向射出面Bl、射入入射區域A2i和A22之光束被 導向射出面B2、射入入射區域A31和A32之光束被導向射出 面B 3 〇 於是’射入入射面A之不相鄰之互異之複數入射區域 之光束被導向各射出面Β1、β2、B3,將那些光束相加後自 各射出面Bl、B2、B3射出。 因此’射入入射面A之光束在入射面a内有不勻,也藉 著加上射入位於遠離位置之2個入射區域之光束而將不勻 平均化,自各射出面Bl、B2、B3射出不勻減少之光束。 尤其如圖4所不’在相對於入射面a之中心彼此位於 反侧之2個入射區域成組的釦 ^ 一 、 Λ ^ 旧和一個射出面對應之情況,如 圖7所不’被量測物Q之配来斗主^ 。, 九特性係上下非對稱之情況,也 措者加上2個入射區域之感本曰 4九I,抵消配光特性之非對稱 性,和束光纖22之轉動角声# $ > 将η度位置無關的自各射出面射出光200303416 V. Description of the invention (7) The amplifying section 24 amplifies the electric signal output from the photoelectric conversion section 23 to a predetermined level. In FIG. 3, the bundle optical fiber 22 is divided into three at the middle portion in the axial direction, and the light beams incident on the incident surface A are separately emitted to the three exit surfaces B1, B2, and B3. As shown in FIG. 4, the incident surface A of the bundle optical fiber 2 is divided into six fan-shaped incident areas A11, A1 2, A 2 1, A 2 2 and A 3 1, A 3 2. It can be seen from FIG. 4 that the incident areas A11 and A1 2, the incident areas A 2 1 and A 2 2, and the incident areas A 3 1 and A 3 2 are located at positions symmetrical to each other about the optical axis l as a center. The light beams entering these two incident areas located at point-symmetrical positions are emitted from the same exit surface. That is, the light beams entering the incident areas A i 1 and A1 2 are guided to the exit surface B1, the light beams entering the incident areas A2i and A22 are directed to the exit surface B2, and the light beams entering the incident areas A31 and A32 are directed to the exit surface B 3 〇Then, the light beams entering the non-adjacent and different plural incident areas of the incident surface A are guided to the exit surfaces B1, β2, and B3, and those beams are added out from the exit surfaces B1, B2, and B3. Therefore, 'the light beam incident on the incident surface A has unevenness in the incident surface a, and the unevenness is also averaged by adding the light beams incident on the two incident regions located away from each other, and the light is emitted from each of the emission surfaces Bl, B2, and B3 A light beam with reduced unevenness is emitted. In particular, as shown in FIG. 4, the two incident areas that are located on the opposite side of each other with respect to the center of the incident surface a are grouped by a pair of buckles ^ I, Λ ^ old and one exit surface, as shown in FIG. 7.物 Q 的 配 来 斗 主 ^. Nine characteristics are the case of up and down asymmetry, and the feeling of 2 incident areas is added to this, which is called 4 I, which cancels the asymmetry of the light distribution characteristics and the rotation angle sound of the optical fiber 22 # $ > η 度Position-independent light emission from each exit surface

2201-5287-Pf(Nl).ptd 第 2003034162201-5287-Pf (Nl) .ptd version 200303416

五、發明說明(8) 量大致相同之光束。因此,光電轉換部2 3之各感光感剛哭 23 2a〜c輸出之電氣信號不會受到被量測物q之配光特性係^ 非對稱性影響,因而,量測值之精度可提高。 μ 此外’在圖4 ’各入射區域a 1 1〜A 3 2成為由直線和圓弧 包圍之扇形,但是實際上因利用多條光纖素線之端面形成 各入射區域,入射區域之邊界未必是漂亮之直線和圓弧。 例如’在邊界部分相鄰之入射區域也可能彼此侵入對 手侧。 、 在上述之實施例,位於點對稱之位置之2個入射區域 和一個射出面對應,但是如圖5(A)所示,使位於係以每隔 30度之中心角劃分之點對稱之位置之4個入射區域和一個 射出面對應也可。即,在圖5(A),使4個入射區域AU、 A12、A13、A14和射出面B1對應,使4個入射區域A21、八22 、A23、A24和射出面B2對應,使4個入射區域A31、A32 可 二A3丄和射出面B3各自對應也可。於是,使位於點對稱 =位置之2 ·η(η係整數)個入射區域和—個射出面對應也 此外’使不在點對稱位置之複數入 加U山 面對應也可。例如,使以#盖I幺 區或和一個射出 J ^ 便以光軸[為中心位於耸fe η (η係3以上之整數)個人A 七 、寺角度位置之 ^ ,枯故射區域和一個射出面對應也可。 使隹不在點對稱位置但是位於 μ5. Description of the invention (8) Beams of approximately the same amount. Therefore, the electrical signals output by each of the light-sensitive sensors 23 of the photoelectric conversion unit 23 are not affected by the asymmetry of the light distribution characteristics of the object q, and therefore, the accuracy of the measurement value can be improved. μ In addition, in FIG. 4, each incident area a 1 1 to A 3 2 has a fan shape surrounded by a straight line and an arc. However, in fact, each incident area is formed by the end faces of a plurality of optical fiber prime lines, and the boundary of the incident area may not necessarily be Beautiful straight lines and arcs. For example, 'the incident areas adjacent to each other in the boundary portion may invade the opposite side of each other. In the above-mentioned embodiment, the two incident areas at the point-symmetrical positions correspond to one exit surface, but as shown in FIG. 5 (A), the positions are symmetrical at the points divided by the central angle every 30 degrees. Four of the incident areas may correspond to one exit surface. That is, in FIG. 5 (A), the four incident areas AU, A12, A13, and A14 correspond to the exit surface B1, and the four incident areas A21, eight 22, A23, A24, and the exit surface B2 correspond to four incident areas. The areas A31 and A32 may correspond to A3 丄 and the emitting surface B3, respectively. Therefore, it is also possible to correspond to 2 · η (η integers) incident areas and one exit plane located at point symmetry = position. In addition, it is also possible to correspond to a plurality of points that are not at the point symmetry position and add U-planes. For example, let # 盖 I 幺 区 or a shot J ^ be centered on the optical axis [at the center of the fe η (η is an integer of 3 or more). Personal A VII. The angle of the temple ^, the shot area and a Correspondence of injection surface is possible. So that 隹 is not in point symmetry but is in μ

内之不句平均化之位置之複數C射面A 也可。例如,如圖5(B)戶斤*,使在人身H個射出面對應 數入射區域和一個射+ ^ ώ ^ 射面A隨機配置之複 们射出面對應也可。尤其,在人射區域之The plural C-radiation plane A of the position where the inner sentences are averaged is also acceptable. For example, as shown in Fig. 5 (B), the number of incident areas corresponding to the H emission surfaces on the human body and one injection + ^ ^ ^ randomly arranged multiple injection surfaces A can also correspond. Especially in the shooting area

第11頁 200303416___ 五、發明說明(9) — ^--- 個數充分大之情況,光纖素線變成隨機配置之隨機分割 (隨機劃分)。在這些情況,和各射出面對應之入射區域之 總面積係彼此相同較好。 此外,在圖5(B)所示之例子,構成束光纖22之各自之 光纖之端面係一個入射區域,那些光纖隨機八社 於3個射出面B之其中之一。在圖5(B),複數人射‘域;;厂 、A12、A13、…和一個射出面B1對應,一樣的入射區域 A21、A2 2、A23、…和一個射出面B2對應,入射區域A31、 A3 2、A33、…和一個射出面B3對應。這些入射區域A1 i、 A1 2、A1 3、…隨機配置於入射面A。入射區域A2 1、A22、 A23、…及入射區域A31、A32、A33、···也一樣的各自隨機 配置於入射面A。 在本實施例,在光分岐裝置上使用光纖,但是使用例 如光導管等之具相同功能之別的光學構件也可。 回到圖2,量測器本體3由A/D轉換部31、資料記憶體 3 2、資料處理部3 3、顯示部3 4、操作輸入部3 5以及控制部 36等構成。 A/D轉換部31將自量測頭2輸入之電氣信號SX、SY、SZ 轉換成數位之量測資料DX、DY、DZ。資料記憶體32記憶自 A/D轉換部31輸出之量測資料DX、DY、DZ、校正資料KX、 KY、KZ以及其他之資料。資料處理部33使用資料記憶體32 所記憶之量測資料計算三刺激值、xyY、Τ ΛιινΥ等。 例如,使用校正資料KX、KY、KZ依據下式計算三刺激 值X、Y、Z。Page 11 200303416___ V. Description of the invention (9) — ^ --- When the number is sufficiently large, the fiber primes become randomly divided randomly (random division). In these cases, it is preferable that the total areas of the incident areas corresponding to the respective exit surfaces are the same as each other. In addition, in the example shown in Fig. 5 (B), the end face of each of the optical fibers constituting the bundle optical fiber 22 is an incident area, and those optical fibers are randomly distributed in one of the three exit surfaces B. In FIG. 5 (B), a plurality of people shoot 'fields ;; factory, A12, A13, ... correspond to one exit surface B1, and the same incident area A21, A2 2, A23, ... correspond to one exit surface B2, and the incident area A31 , A3 2, A33, ... correspond to an injection surface B3. These incident areas A1 i, A1 2, A1 3,... Are randomly arranged on the incident surface A. The incident areas A2 1, A22, A23, ... and the incident areas A31, A32, A33, ... are also randomly arranged on the incident surface A. In this embodiment, an optical fiber is used for the optical branching device, but another optical member having the same function, such as a light pipe, may be used. Returning to FIG. 2, the measuring instrument body 3 is composed of an A / D conversion unit 31, a data memory 3 2, a data processing unit 3, a display unit 3 4, an operation input unit 35, and a control unit 36. The A / D conversion section 31 converts the electrical signals SX, SY, and SZ input from the measuring head 2 into digital measurement data DX, DY, and DZ. The data memory 32 stores measurement data DX, DY, DZ, calibration data KX, KY, KZ and other data output from the A / D conversion section 31. The data processing unit 33 uses the measurement data stored in the data memory 32 to calculate tristimulus values, xyY, T Λινν, and the like. For example, the calibration data KX, KY, and KZ are used to calculate the tristimulus values X, Y, and Z according to the following formula.

2201-5287-Pf(Nl).ptd 第12頁 200303416 五、發明說明(10)2201-5287-Pf (Nl) .ptd Page 12 200303416 V. Description of the invention (10)

\二 KX ·DX Y二 KY · DY Z- KZ ·DZ 顯示部3 4顯示運算結果。操作輸入部3 5由使用者操作 ,輸入關於量測之各種資訊(量測之指示、顯示模式之設 定、量測範圍等)。控制部3 6集中的控制量測頭2之動作及 量測器本體3内之各部之動作與處理。 其次使用圖8之流程圖說明色度計1之量測動作。 在圖8,首先,如圖1所示,將量測頭2設成朝向係被 量測物Q之液晶面板之被量測區域A R ( #丨丨)。自未圖示之圖 案產生器向液晶面板傳送影像信號,在液晶面板之顯示面 HG顯示既定之量測用影像(#丨2 )。 顯示量測用影像時,自各感光感測器2 32a〜c輸出關於 三刺激值之3個感光信號SX、SY、SZ。用放大部24感光信 號放大至既定之位準後,輸入量測器本體3。在量測器本 體3 ’用A / D轉換部3 1將感光信號轉換成量測資料d X、d γ、 DZ後,儲存於資料記憶體32(#13)。 接著’資料處理部3 3自資料記憶體3 2讀出量測資料及 校正資料後,計算量測用影像之三刺激值、色度座標、亮 度、相關色溫等(# 1 4)。在顯示部3 4顯示計算結果(# 1 5 )。 在上述之實施例,在射入束光纖2 2之入射面A之光量 有不勻,也藉著加上射入位於遠離位置之2個入射區域之 光束而將不勻平均化。因此,未發生如以往之量測頭2 (光 學系KK1)之轉動所引起之量測值(三刺激值)之變化。因\ 2 KX · DX Y 2 KY · DY Z- KZ · DZ The display section 34 displays the calculation result. The operation input section 35 is operated by the user to input various information about measurement (instructions for measurement, setting of display mode, measurement range, etc.). The control unit 36 centrally controls the operation of the measuring head 2 and the operations and processing of each unit in the measuring unit body 3. Next, the measurement operation of the colorimeter 1 will be described using the flowchart of FIG. 8. In FIG. 8, first, as shown in FIG. 1, the measuring head 2 is set so as to face the measurement area A R (# 丨 丨) of the liquid crystal panel of the measurement object Q. An image signal is transmitted from the unillustrated pattern generator to the liquid crystal panel, and the predetermined measurement image (# 丨 2) is displayed on the display surface HG of the liquid crystal panel. When a measurement image is displayed, three photosensitive signals SX, SY, and SZ regarding the three stimulus values are output from each of the photosensitive sensors 2 32a to c. The amplified signal is amplified to a predetermined level by the amplifying section 24, and then input to the measuring device body 3. After the measuring device body 3 'uses the A / D conversion section 31 to convert the photosensitive signal into measurement data d X, d γ, and DZ, it is stored in the data memory 32 (# 13). Next, the “data processing section 33” reads out the measurement data and the calibration data from the data memory 32, and calculates the tristimulus value, chromaticity coordinates, brightness, and correlated color temperature of the measurement image (# 1 4). The calculation result (# 1 5) is displayed on the display section 3 4. In the above-mentioned embodiment, the amount of light on the incident surface A of the incident optical fiber 22 is uneven, and the unevenness is also averaged by adding the light beams that are incident on the two incident areas located away from each other. Therefore, the measurement value (tristimulus value) caused by the rotation of the conventional measurement head 2 (optical department KK1) does not occur. because

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200303416 五、發明說明(π) 而,未受到被量測物Q之配光特性等影響,進行高精度之 量測,可正確的量測顏色。 其次說明量測頭2之別的實施例之光學系ΚΚ2之構造。 圖9係表示量測頭2之別的實施例之光學系ΚΚ 2之構造 圖,圖1 0係表示在圖9之光學系ΚΚ2自被量測物Q出來之光 至入射面Α之路徑圖。 在圖9,光學系KK2由物鏡103、光圈止鐵104、視野止 鐵105、中繼透鏡106以及束光纖22等構成。 物鏡103將來自被量測物Q之光束聚光於視野止鐵105 之位置而令成像。中繼透鏡1 0 6將成像於視野止鐵1 〇 5之位 置之像導至束光纖22之入射面A。光圈止鐵104配置於物鏡 1 0 3之後方,只有通過了光圈止鐵1 〇 4之光束往中繼透鏡 1 0 6。束光纖2 2和以上所說明的相同即可。 中繼透鏡106配置於光圈止鐵1〇4和入射面A變成在光 學上共軛之關係之位置。換言之,束光纖2 2對於中繼透鏡 1 0 6配置成入射面A和光圈止鐵1 〇 4變成共輥之關係。 使用這種光學系K K 2之情況,射入入射面a之位置也按 照自被1出來之光束之射出角α而定。 即,如圖1 0所示,自被量測區域…之某點出來後射入 入射面A之光束之中,上半部之光束(以斜線表示之部分) 射入入射面A之下半部,下半部之光束(無斜線之部 入入射面A之上半部。 射 而,在使用這種光學系KK2之情況,也藉著使用以 所况明之束光纖22,未受到被量測物q之配光特性等影響200303416 V. Description of the invention (π) In addition, it is not affected by the light distribution characteristics of the measured object Q, and it can accurately measure color by performing high-precision measurement. Next, the structure of the optical system KK2 in another embodiment of the measuring head 2 will be described. FIG. 9 is a structural diagram of an optical system KK 2 showing another embodiment of the measuring head 2, and FIG. 10 is a path diagram of light from the object Q to the incident surface A in the optical system KK 2 of FIG. 9. . In FIG. 9, the optical system KK2 is composed of an objective lens 103, an aperture stop 104, a field stop 105, a relay lens 106, a bundle optical fiber 22, and the like. The objective lens 103 condenses the light beam from the object to be measured Q at the position of the field stop 105 and forms an image. The relay lens 106 guides the image formed at the position of the field stop 105 to the incident surface A of the bundle optical fiber 22. The aperture stop 104 is arranged behind the objective lens 103, and only the light beam that has passed through the aperture stop 104 goes to the relay lens 106. The bundle optical fiber 22 may be the same as described above. The relay lens 106 is disposed at a position where the aperture stop 104 and the incident surface A become optically conjugated. In other words, the bundle optical fiber 22 is arranged so that the incident surface A and the diaphragm stop iron 104 have a common roll relationship with the relay lens 106. In the case of using this optical system K K 2, the position of the incident light incident on the incident surface a also depends on the exit angle? That is, as shown in FIG. 10, after a certain point of the measurement area ... comes out of the light beam incident on the incident surface A, the upper half of the light beam (the part indicated by the oblique line) is incident on the lower half of the incident surface A (The part without the oblique line enters the upper half of the incident surface A.) In the case of using this optical system KK2, the optical fiber 22 is used without being affected by the beam. Effects of light distribution characteristics of the test object q

200303416 五、發明說明(12) ’可進行高精度之量測。 在上述之實施例,表示具有3個射出面B之束光纖22之 例子,但是係具有2個或4個以上之射出面B的也可。又, 關於入射面A係不是一個也可。入射面A之入射區域之劃分 之方法、形狀、個數、束光纖2 2之構造、材質、形狀等設 為上述以外之各種的也可。 在上述之實施例,在量測頭2之光學系上可採用具有 將自被量測物Q出來之光導向入射面A之功能之其他各種的 構造。表示在量測頭内藏了光學系KK 1、2之例子,作是係 内藏於量測頭以外之各種機器的也可,又以獨立之:: 構成也可。 九子糸 一 在上述之實施例,光電轉換部23在構造上在紅光、綠 光、監光之波長區域具有大的靈敏度,但是設為與 之光譜靈敏度的也可。量測器本體3之功能利用執行^;各同 之程式之CPU以軟體實現也可,利用硬體電路實二I田 或利用其組合實現也可。 可’ 應用於色 光學機器 在上述之實施例,表示將本發明之光學叢置 度計1之例子,但是可應用於色度計1以外之各種 或量測機器。 、 此外,按照本發明之主旨可適當的變更量測頭2、旦 測益本體3或色度計1之整體或各部之構造、電路、、里 容、處理順序、處理時序、各種數值等。本發明可二== 液晶面板以外之各種被量測物之量測。 … ' 【發明效果】200303416 V. Description of the invention (12) ′ It can measure with high accuracy. In the above-mentioned embodiment, an example of the bundle optical fiber 22 having three emitting surfaces B is shown, but it is also possible to have two or more emitting surfaces B. It is not necessary to have only one incident surface A system. The method, shape, number, and structure, material, and shape of the incident area A of the incident area A may be set to various other than the above. In the above-mentioned embodiment, the optical system of the measuring head 2 may adopt other various structures having a function of directing the light from the object to be measured Q to the incident surface A. This example shows that the optical system KK 1 and 2 are embedded in the measuring head. It can be used for various devices other than the measuring head, and it can also be an independent :: structure. Nine sons and sisters 1. In the above embodiment, the photoelectric conversion unit 23 has a large sensitivity in the wavelength region of red light, green light, and monitor light, but it may be set to have a spectral sensitivity. The function of the measuring instrument body 3 can be implemented by using ^; the CPU of each program can be realized by software, and it can also be realized by hardware circuits or by a combination thereof. Applicable to color optical devices In the above-mentioned embodiment, the example of the optical cluster meter 1 according to the present invention is shown, but it can be applied to various or measuring devices other than the color meter 1. In addition, according to the gist of the present invention, the structure, circuit, contents, processing sequence, processing sequence, various values, etc. of the measuring head 2 or the whole or each part of the measuring body 3 or the colorimeter 1 can be changed as appropriate. The present invention can measure two kinds of objects to be measured other than a liquid crystal panel. … '[Inventive effect]

200303416200303416

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圖1係表示本發明之實施例之二 之外觀之立體圖。 二刺激值型光電色度計 圖2係表示三刺激值型光電 塊圖。 又冲之功能性構造之方 圖3係表示量測頭之光學系 之入射區域 圖4係表示在束光纖之入射 =圖 圖。 耵面所劃分 之 圖5(A)〜5(B)係表示所劃分之入射 圖6係表示自被量測物出來之光至σσ或之別例之圖。 圖7係表示被量測物之配氺 Ζ 射面之路彳呈圖。 70 7寸性為非對猫& 。 F對%性之情況例 圖8係表示色度計之量澳j 圖9係表示量測頭之別的 圖10係表示在圖9之光學 射面A之路徑圖。 動作之流程圖。 實施例之光學系之構造圖 糸自被量測物出來之光至 圖11係表不以往在入射 符號說明 面所劃分之入射區域之圖 卜色度計(三刺激值型光電色度計) 2〜量測頭(量測用光學裴置)° ’ 21〜物鏡(聚光裝置); 2 2〜束光纖(光分岐裝置); 23〜光電轉換部(感光裝置); 3 3〜資料處理部(運算裝置); 10 3〜物鏡(第一聚光裝置);Fig. 1 is a perspective view showing the appearance of a second embodiment of the present invention. Two-stimulus-type photoelectric colorimeter Figure 2 shows a tristimulus-type photoelectric block diagram. Rectangular functional structure Figure 3 shows the incident area of the optical system of the measuring head. Figure 4 shows the incidence of the optical fiber in the bundle. Figures 5 (A) to 5 (B) are the incident incidents divided by the plane. Figure 6 is a diagram showing other examples of light from the measured object to σσ or above. FIG. 7 is a view showing a road surface of a distribution surface of a measured object. 70 7-inch sex is not right for cats & Example of F vs.% property Fig. 8 shows the amount of colorimeter j Fig. 9 shows the difference of the measuring head Fig. 10 shows the path diagram on the optical surface A of Fig. 9. Flow chart of actions. Structure diagram of the optical system of the embodiment 糸 The light from the object to be measured to FIG. 11 is a colorimeter (three stimulus value photoelectric colorimeter) showing the incident area divided on the explanation surface of the incident symbol in the past. 2 ~ measuring head (optical measurement for measurement) ° '21 ~ objective lens (condensing device); 2 2 ~ bundle optical fiber (optical divergence device); 23 ~ photoelectric conversion unit (photosensitive device); 3 3 ~ data processing (Computing device); 10 3 ~ objective lens (first condensing device);

2201-52S7-Pf(Nl).ptd 200303416 圖式簡單說明 104 105 106 KK1 光圈止鐵; 視野止鐵; 中繼透鏡(第二聚光裝置); KK2〜光學系(量測用光學裝置) A〜入射面; A 1 1〜A 3 2入射區域; B〜射出面; Q〜被量測物。2201-52S7-Pf (Nl) .ptd 200303416 Brief description of the diagram 104 105 106 KK1 Aperture stop iron; Field of view stop iron; Relay lens (second condensing device); KK2 ~ Optical system (Measuring optical device) A ~ Incident surface; A 1 1 ~ A 3 2 incident area; B ~ exit surface; Q ~ measured object.

2201-5287-Pf(Nl).ptd 第18頁2201-5287-Pf (Nl) .ptd Page 18

Claims (1)

200303416 六、申請專利範圍 ____ 丨·一種量測用光學裝置,包括:光分岐裝i, =入入射面之來自被量測物之光分岐後射出之複數射出將 其特徵在於: 在構造上將該入射面劃分成複數入射區域,自 該射出面射出射入不相鄰之彼此相異之複數入射自之 2·如申请專利範圍第丨項之量測用光學裝置,发 該量測用光學裝置包括將來自被之、中’ 置,將該光分岐裝置配詈此兮λ仏 尤來尤之I光裝 之像側主點和其焦距大致相等之距離之位置。Τ先衣置 3.如申請專利範圍第i項之量測用光學裝置, 該量測用光學裝置包括: ”中’ 第;:聚光裝置,將來自被量測物之光聚光; 光圈jh鐵’配置於古女笛 ^ . 第一,…” 弟—聚先裝置之後方;以及 弟一水先衣置,將通過了該光圈止鐵之光聚光· 该光分岐裝置配置於相對於該第二聚光 又 和該光圈止鐵變成共軛之關係之位置。 、。/入射面 並範圍第1 '2或3項之量測用光學 八中’各自和各自之該射出面對應 此相對於在該人射面之中心點對稱之位置。射£域位於彼 5第i '2或3項之量測用光 射面位於隨機之位置.。面對應之稷數入射區域在該入 6.—種量測用光學裝置’其特徵在於包括:200303416 VI. Scope of patent application ____ 丨 · An optical device for measurement, including: optical branching device i, = complex emission after the light branching from the measured object that enters the incident surface is characterized by: The incident surface is divided into a plurality of incident areas, and a plurality of non-adjacent complex incidents are emitted from the emitting surface. 2. If the optical device for measurement of item 丨 of the patent application scope is issued, the measurement The optical device includes a position from which the optical divergence device is arranged, and the optical divergence device is arranged at a distance of approximately equal to the principal point of the image side of the optical device and the focal length thereof. Τ 先 衣装 3. If the optical device for measurement in item i of the patent application scope, the optical device for measurement includes: "Medium" No. :: Concentrating device that condenses the light from the object to be measured; aperture jh iron 'is placed in the ancient female flute ^. First, ... ”Brother—the first device is behind the device; and Brother Yishui is the first to place the light to condense the light that has passed through the aperture to stop the iron. The second spotlight is in a conjugate relationship with the diaphragm stop iron. . / Incoming plane and measuring optics in the range 1'2 or 3 of the measurement optics Each of Bazhong's corresponds to the respective exit plane This is a symmetrical position with respect to the center point of the incident plane. The radiation field is located at the measurement light beam of item i'2 or 3 on the other side. The radiation surface is located at a random position. The plane of incidence of the unit number is in this 6.-A measuring optical device ', which is characterized by: 2201-5287-Pf(Nl).ptd 第19頁 200303416 六、申請專利範圍 光分岐裝置,在構造上具有將射入入射面之來自被量 測物之光分岐後射出之複數射出面,將該入射面劃分成複 數入射區域,自各自之該射出面射出射入不相鄰之彼此相 異之複數入射區域; 感光裝置,和該光分岐裝置之各自之射出面相向的配 置,將射入該入射面之光分解成色成分後轉換為電氣信號 ;以及 計算裝置,依照自該感光裝置輸出之電氣信號計算三 刺激值。2201-5287-Pf (Nl) .ptd Page 19, 200303416 6. The patent application scope optical divergence device has a structure that has a complex exit surface that emits the divergent light from the measured object that is incident on the incident surface. The incident surface is divided into a plurality of incident areas, and from each of the emitting surfaces, a non-adjacent complex incident area that is different from each other is emitted; the photosensitive device and the respective emitting surfaces of the optical divergence device are arranged to face each other, and will be incident on the The light on the incident surface is decomposed into color components and converted into electrical signals; and a computing device calculates a tristimulus value based on the electrical signals output from the photosensitive device. 2201-5287-Pf(Nl).ptd 第20頁2201-5287-Pf (Nl) .ptd Page 20
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