JPH10160571A - Spectrophotometer - Google Patents

Spectrophotometer

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Publication number
JPH10160571A
JPH10160571A JP8334998A JP33499896A JPH10160571A JP H10160571 A JPH10160571 A JP H10160571A JP 8334998 A JP8334998 A JP 8334998A JP 33499896 A JP33499896 A JP 33499896A JP H10160571 A JPH10160571 A JP H10160571A
Authority
JP
Japan
Prior art keywords
light
integrating sphere
window
sample
light beam
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP8334998A
Other languages
Japanese (ja)
Inventor
Osamu Ando
修 安藤
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Shimadzu Corp
Original Assignee
Shimadzu Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Shimadzu Corp filed Critical Shimadzu Corp
Priority to JP8334998A priority Critical patent/JPH10160571A/en
Publication of JPH10160571A publication Critical patent/JPH10160571A/en
Pending legal-status Critical Current

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Abstract

(57)【要約】 【課題】 積分球による測定精度を向上する。 【解決手段】 積分球10には試料測定光束LSの入射
窓11、反射窓12、光検出窓13を設け、拡散反射光
を試料側光検出器23にて検出する。一方、参照光束L
Rは積分球10の外側に設けた参照側光検出器24にて
検出する。そして、両検出信号を加算アンプ27により
加算した後に演算処理し反射率等を算出する。これによ
り、積分球の開口率を小さくできるので拡散光の捕集効
率がよくなると共に、窓が少ないので積分球の設計が容
易になる。
(57) [Summary] [PROBLEMS] To improve measurement accuracy by an integrating sphere. SOLUTION: An integrating sphere 10 is provided with an entrance window 11, a reflection window 12, and a light detection window 13 for a sample measurement light beam LS, and diffusely reflected light is detected by a sample-side photodetector 23. On the other hand, the reference beam L
R is detected by a reference-side photodetector 24 provided outside the integrating sphere 10. Then, after adding the two detection signals by the addition amplifier 27, an arithmetic processing is performed to calculate the reflectance and the like. Thereby, the aperture ratio of the integrating sphere can be reduced, so that the efficiency of collecting the diffused light is improved, and the design of the integrating sphere is facilitated because the number of windows is small.

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】本発明は分光光度計に関し、
特に積分球測定部を用いたダブルビーム式の分光光度計
に関する。
The present invention relates to a spectrophotometer,
In particular, it relates to a double beam type spectrophotometer using an integrating sphere measuring unit.

【0002】[0002]

【従来の技術】図2は、従来の分光光度計における積分
球測定部の構成を示す図である。この測定部には、同一
光源から発した光を二分割した試料測定光束LS及び参
照光束LRが近接して略平行に導入される。各光束LS、
LRはそれぞれ反射鏡21、22で反射され、試料測定
光束入射窓31及び参照光束入射窓34を通して積分球
30内部に導びかれる。積分球30は反射率の良好な内
面を有しており、導入された両光束LS、LRはそれぞれ
試料測定光束反射窓32及び参照光束反射窓35の開口
に至る。反射窓32、35の外側至近の測定試料載置位
置a及び参照試料載置位置bにはそれぞれ例えば未知試
料及び標準白板が配置され、その未知試料及び標準白板
で鏡面反射した光は積分球30内部を図2に示すように
進み、鏡面光除去窓36から積分球30外部に取り出さ
れる。
2. Description of the Related Art FIG. 2 is a diagram showing a configuration of an integrating sphere measuring section in a conventional spectrophotometer. A sample measurement light beam LS and a reference light beam LR, which are obtained by splitting light emitted from the same light source into two, are introduced into this measuring unit in a nearly parallel manner. Each light beam LS,
LR is reflected by the reflecting mirrors 21 and 22, respectively, and guided to the inside of the integrating sphere 30 through the sample measurement light beam entrance window 31 and the reference light beam entrance window. The integrating sphere 30 has an inner surface with good reflectivity, and the introduced light beams LS and LR reach the openings of the sample measurement light beam reflection window 32 and the reference light beam reflection window 35, respectively. For example, an unknown sample and a standard white plate are respectively disposed at the measurement sample mounting position a and the reference sample mounting position b near the outside of the reflection windows 32 and 35, and the light specularly reflected by the unknown sample and the standard white plate is integrated by the integrating sphere 30. The inside proceeds as shown in FIG. 2 and is taken out of the integrating sphere 30 through the mirror light removal window 36.

【0003】一方、未知試料及び標準白板で拡散反射し
た光は種々の方向に進み、積分球30の内面で反射を繰
り返す。積分球30の適宜の箇所には光検出窓33が開
口され、拡散反射光の大部分は光検出窓33から出てそ
の外側至近に配置された光検出器23の受光面に到達す
る。光検出器23は受光光の強度に応じた検出信号を出
力し、この信号はアンプ25で増幅された後に演算処理
部28に入力される。
On the other hand, light diffusely reflected by the unknown sample and the standard white plate travels in various directions, and is repeatedly reflected on the inner surface of the integrating sphere 30. A light detection window 33 is opened at an appropriate position of the integrating sphere 30, and most of the diffuse reflected light exits from the light detection window 33 and reaches a light receiving surface of the light detector 23 disposed close to the outside. The photodetector 23 outputs a detection signal corresponding to the intensity of the received light, and the signal is amplified by the amplifier 25 and then input to the arithmetic processing unit 28.

【0004】上記構成のダブルビーム式の積分球測定部
では、以下のように試料の拡散反射率(又は透過率)を
測定する。まず、測定試料載置位置a及び参照試料載置
位置bに、それぞれ100%拡散反射の標準白板を置
く。試料測定光束LS及び参照光束LRは交互に照射され
るので、光検出器23は試料測定光束LSに対する10
0%拡散光の検出信号S(100)と参照光束LRに対する1
00%拡散光の検出信号Rとを交互に出力する。この信
号に基づき、演算処理部28は両検出信号の比D(100)
=S(100)/Rを算出する。次に、測定試料載置位置a
に測定対象の未知試料を置き、光検出器23において試
料測定光束LSに対する未知試料の拡散光の検出信号S
(S)と参照光束LRに対する100%拡散光の検出信号R
とを得る。この信号に基づき、演算処理部28は両検出
信号の比D(S)=S(S)/Rを算出し、更にD(100)とD
(S)の比T=D(S)/D(100)=S(S)/S(100)を計算す
ることにより反射率を算出する。
The double-beam integrating sphere measuring section having the above-described configuration measures the diffuse reflectance (or transmittance) of a sample as follows. First, a standard white plate having 100% diffuse reflection is placed at each of the measurement sample mounting position a and the reference sample mounting position b. Since the sample measurement light beam LS and the reference light beam LR are alternately irradiated, the photodetector 23 sets the 10
1% for the detection signal S (100) of the 0% diffused light and the reference light beam LR.
The detection signal R of the 00% diffused light is output alternately. Based on this signal, the arithmetic processing unit 28 determines the ratio D (100) of the two detection signals.
= S (100) / R is calculated. Next, the measurement sample mounting position a
An unknown sample to be measured is placed in the detector, and the detection signal S of the diffused light of the unknown sample with respect to the sample measurement light beam LS is detected by the photodetector 23.
(S) and a detection signal R of 100% diffused light for the reference light beam LR
And get Based on this signal, the arithmetic processing unit 28 calculates the ratio D (S) = S (S) / R between the two detection signals, and further calculates D (100) and D (100).
The reflectance is calculated by calculating the ratio of (S) T = D (S) / D (100) = S (S) / S (100).

【0005】[0005]

【発明が解決しようとする課題】上記構成において積分
球30は拡散光を効率よく光検出窓33に集めることが
目的であるから、球に近い形状であるほど理想的であ
り、開口率(内面積に対する開口面積の比率)が小さい
ほど好ましい。しかしながら、上述のように従来の積分
球測定部では積分球30に多くの窓を開口させなければ
ならず、開口率が大きくなって拡散光の捕集効率が劣化
してしまう。
In the above configuration, since the purpose of the integrating sphere 30 is to collect the diffused light efficiently in the light detection window 33, the shape closer to the sphere is more ideal, and the aperture ratio (the The smaller the ratio of the opening area to the area, the better. However, as described above, in the conventional integrating sphere measuring section, many windows must be opened in the integrating sphere 30, so that the aperture ratio increases and the efficiency of collecting diffused light deteriorates.

【0006】また、この種の分光光度計では一般に直径
が60〜200mm程度の積分球が使用されるが、この
ような積分球に上述の如く多数の窓を最適の位置に設け
る設計はかなり困難である。すなわち、試料や標準白板
における光の入反射角度が大きいと偏光方向による拡散
反射率の相違が大きくなり正確な測定が行なえなくなる
ため、その入反射角度は小さい(通常10°程度以下)
ほうが好ましい。このような入反射角度や両光束LS、
LRの間隔等の諸制約条件の下に、試料測定光束入射窓
31、参照光束入射窓34、試料測定光束反射窓32、
参照光束反射窓35及び共通の鏡面光除去窓36を配置
しなければならない。
Further, in this type of spectrophotometer, an integrating sphere having a diameter of about 60 to 200 mm is generally used, but it is quite difficult to design such an integrating sphere with a large number of windows at optimal positions as described above. It is. That is, when the incident angle of light on a sample or a standard white plate is large, the difference in diffuse reflectance depending on the polarization direction becomes large, and accurate measurement cannot be performed. Therefore, the incident angle is small (usually about 10 ° or less).
More preferred. Such incident angles of reflection and both light beams LS,
Under various constraints such as the interval of LR, the sample measurement beam entrance window 31, the reference beam entrance window 34, the sample measurement beam reflection window 32,
A reference beam reflection window 35 and a common mirror light removal window 36 must be provided.

【0007】本発明は上記課題を解決するために成され
たものであり、その目的とするところは、積分球測定部
の測定精度や感度を向上すると共に、積分球の設計を容
易にすることができる分光光度計を提供することにあ
る。
SUMMARY OF THE INVENTION The present invention has been made to solve the above problems, and an object of the present invention is to improve the measurement accuracy and sensitivity of an integrating sphere measuring section and to facilitate the design of an integrating sphere. It is to provide a spectrophotometer which can be used.

【0008】[0008]

【課題を解決するための手段】上記課題を解決するため
に成された本発明は、試料測定光束及び参照光束を用い
るダブルビーム型の分光光度計において、 a)光入射窓から導入した試料測定光を光反射窓の外側近
傍に配置した試料に照射し、該試料からの拡散反射光を
内面に反射させて光検出窓に導くように、光入射窓、光
反射窓及び光検出窓を適宜の位置に開口した積分球と、 b)前記光検出窓を通して積分球の外側に取り出された光
を検出する第1の光検出手段と、 c)前記積分球の外部において参照光束を検出する第2の
光検出手段と、 d)第1及び第2の光検出手段の検出信号を基に、試料の
光学的な特性を示す指標値を算出する演算手段と、を備
えることを特徴としている。
SUMMARY OF THE INVENTION In order to solve the above-mentioned problems, the present invention provides a double beam type spectrophotometer using a sample measuring light beam and a reference light beam. The light incident window, the light reflection window and the light detection window are appropriately illuminated so that the light is irradiated on the sample arranged near the outside of the light reflection window, and the diffuse reflection light from the sample is reflected on the inner surface and guided to the light detection window. B) first light detection means for detecting light taken out of the integrating sphere through the light detection window; and c) detecting a reference light beam outside the integrating sphere. And d) calculating means for calculating an index value indicating an optical characteristic of the sample based on the detection signals of the first and second light detecting means.

【0009】[0009]

【発明の実施の形態】本発明に係る分光光度計では、試
料測定光束のみが光入射窓を通して積分球内部に導入さ
れ、光反射窓の外側近傍に配置されている試料に当たっ
て反射する。拡散反射光は種々の方向に進み、積分球の
内面で反射を繰り返して光検出窓に到達すると積分球か
ら出て第1の光検出手段により受光される。従って第1
の光検出手段は、試料からの拡散反射光の強度に応じた
検出信号を出力する。一方、積分球の外側に配置された
第2の光検出手段は試料測定光束とは相違する光路を通
る参照光束を受光し、この受光光の強度に応じた検出信
号を出力する。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS In a spectrophotometer according to the present invention, only a sample measuring light beam is introduced into an integrating sphere through a light incident window, and reflects on a sample arranged near the outside of a light reflecting window. The diffusely reflected light travels in various directions, repeats reflection on the inner surface of the integrating sphere, and when it reaches the light detection window, exits the integrating sphere and is received by the first light detecting means. Therefore the first
The light detection means outputs a detection signal corresponding to the intensity of the diffuse reflection light from the sample. On the other hand, the second light detecting means disposed outside the integrating sphere receives a reference light beam passing through an optical path different from the sample measurement light beam, and outputs a detection signal corresponding to the intensity of the received light.

【0010】例えば、第1及び第2の光検出手段の出力
信号は加算アンプ等を用いてアナログ的に加算される。
試料測定光束と参照光束とが交互に照射されると、加算
アンプの出力には、試料からの拡散反射光に対応する検
出信号と参照光束に対応する検出信号とが交互に得られ
る。そこで、この両者の検出信号を用いて、演算手段
は、従来と同様に試料の光学的な特性を示す指標値とし
て反射率や透過率を算出する。勿論、第1及び第2の光
検出手段による検出信号をアナログ的に加算せずに、例
えばそれぞれディジタル信号に変換した後に演算処理を
行なってもよい。
For example, the output signals of the first and second light detecting means are added in an analog manner using an adding amplifier or the like.
When the sample measurement light beam and the reference light beam are alternately irradiated, a detection signal corresponding to the diffuse reflection light from the sample and a detection signal corresponding to the reference light beam are alternately obtained at the output of the addition amplifier. Therefore, using these two detection signals, the calculating means calculates the reflectance and the transmittance as index values indicating the optical characteristics of the sample as in the related art. Of course, the arithmetic processing may be performed after, for example, converting the detection signals from the first and second light detection means into digital signals, respectively, without adding them in an analog manner.

【0011】なお、試料からの鏡面反射光を除いた拡散
反射率のみを算出する場合には、試料からの鏡面反射光
を積分球の外部に取り出すための鏡面光除去窓を積分球
の適宜の箇所に設けるようにすればよい。
When only the diffuse reflectance excluding the specular reflection light from the sample is calculated, a specular light removal window for extracting the specular reflection light from the sample to the outside of the integrating sphere is appropriately set. It may be provided at a location.

【0012】[0012]

【発明の効果】本発明に係る分光光度計によれば、積分
球には光入射窓、光反射窓及び光検出窓、更に必要に応
じて鏡面光除去窓の最大4個の窓を設けるのみでよいの
で、従来の積分球と比較して開口率を小さくすることが
できる。このため、拡散反射光を効率よく光検出窓に集
めることができ、測定の精度が向上する。また、積分球
に設ける窓の数が減り且つ窓の位置の制約が緩やかにな
るので、積分球自体の設計が容易になるのみならず、外
部の部品配置の自由度が増し、大きな積分球を用いつつ
測定部を小形にすることができる。
According to the spectrophotometer according to the present invention, the integrating sphere is provided with only a light entrance window, a light reflection window, a light detection window and, if necessary, a maximum of four windows of a specular light removal window. Therefore, the aperture ratio can be reduced as compared with the conventional integrating sphere. For this reason, diffuse reflection light can be efficiently collected in the light detection window, and measurement accuracy is improved. In addition, the number of windows provided on the integrating sphere is reduced and restrictions on the position of the windows are relaxed, so that not only the design of the integrating sphere itself is facilitated, but also the degree of freedom in arranging external parts is increased, and a large integrating sphere is required. The measuring part can be miniaturized while using.

【0013】[0013]

【実施例】以下、本発明に係る分光光度計の一実施例に
ついて図を参照しつつ説明する。図1は本実施例の分光
光度計における積分球測定部の構成図である。積分球1
0には、入射窓11、反射窓12、光検出窓13及び鏡
面光除去窓14がそれぞれ所定位置に開口している。光
検出窓13の外側至近には試料側光検出器23が配置さ
れる一方、積分球10の外側には参照側光検出器24が
配置されている。両光検出器23、24の検出信号はそ
れぞれ試料側アンプ25、参照側アンプ26で増幅され
た後に加算アンプ27にてアナログ的に加算される。加
算アンプ27の出力信号は演算処理部28へ入力されて
いる。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS One embodiment of the spectrophotometer according to the present invention will be described below with reference to the drawings. FIG. 1 is a configuration diagram of an integrating sphere measuring unit in the spectrophotometer of the present embodiment. Integrating sphere 1
At 0, an entrance window 11, a reflection window 12, a light detection window 13, and a specular light removal window 14 are respectively opened at predetermined positions. A sample-side photodetector 23 is arranged near the outside of the light detection window 13, while a reference-side photodetector 24 is arranged outside the integrating sphere 10. The detection signals of the two photodetectors 23 and 24 are amplified by a sample side amplifier 25 and a reference side amplifier 26, respectively, and then added in an analog manner by an addition amplifier 27. The output signal of the addition amplifier 27 is input to the arithmetic processing unit 28.

【0014】図2の従来の分光光度計と同様に、同一光
源から発した光を二分割した試料測定光束LS及び参照
光束LRはこの測定部に近接して略平行に導入される。
試料測定光束LSは反射鏡21で反射され、入射窓11
を通して積分球10内部に導びかれる。この試料測定光
束LSは反射窓12の外側至近の測定試料載置位置aに
置かれた試料に当たり、鏡面反射光は図1に示すように
進んで鏡面光除去窓14から積分球10外部に取り出さ
れる。試料で拡散反射した光は積分球10の内面で反射
を繰り返して光検出窓13に至り、試料側光検出器23
により検出される。一方、参照光束LRは反射鏡22で
反射され後に、直接、参照側光検出器24により検出さ
れる。すなわち、本実施例の構成では、参照光束LRは
積分球10内部を通過しない。
As in the conventional spectrophotometer of FIG. 2, the sample measurement light beam LS and the reference light beam LR obtained by splitting the light emitted from the same light source into two light beams are introduced in substantially parallel to the measuring section.
The sample measurement light beam LS is reflected by the reflecting mirror 21 and is incident on the entrance window 11.
Through the inside of the integrating sphere 10. This sample measurement light beam LS impinges on the sample placed at the measurement sample mounting position a closest to the outside of the reflection window 12, and the specular reflected light proceeds as shown in FIG. It is. The light diffusely reflected by the sample repeatedly reflects on the inner surface of the integrating sphere 10 and reaches the light detection window 13, where the light is detected by the sample-side light detector 23.
Is detected by On the other hand, the reference light beam LR is directly reflected by the reference mirror 24 after being reflected by the reflecting mirror 22. That is, in the configuration of the present embodiment, the reference light beam LR does not pass through the inside of the integrating sphere 10.

【0015】まず、測定試料載置位置aに100%拡散
反射の標準白板を置き、測定を行なう。従来と同様に試
料測定光束LSと参照光束LRとが交互に照射されると、
試料側光検出器23では、試料測定光束LSが照射され
る期間にその試料測定光束LSに対する100%拡散光
の検出信号S(100)が出力され、参照光束LRが照射され
る期間にはその出力は零となる(厳密には暗電流に応じ
た微小ノイズが出力される)。一方、参照側光検出器2
4では、参照光束LRが照射される期間にその参照光束
LRに対する検出信号Rが出力され、試料測定光束LSが
照射される期間にはその出力は零となる。加算アンプ2
7では両検出信号が加算されるので、その出力信号には
試料測定光束LSに対する100%拡散光の検出信号S
(100)と参照光束LRに対する検出信号Rとが交互に現わ
れる。従って、この出力信号に基づいて、演算処理部2
8は両検出信号の比D(100)=S(100)/Rを算出する。
First, a standard white plate having 100% diffuse reflection is placed at the measurement sample mounting position a, and measurement is performed. As before, when the sample measurement light beam LS and the reference light beam LR are alternately irradiated,
The sample-side photodetector 23 outputs a detection signal S (100) of 100% diffused light with respect to the sample measurement light beam LS during a period during which the sample measurement light beam LS is irradiated, and outputs the detection signal S (100) during a period during which the reference light beam LR is irradiated. The output becomes zero (strictly speaking, minute noise corresponding to the dark current is output). On the other hand, the reference side photodetector 2
In 4, the detection signal R for the reference light beam LR is output during the irradiation of the reference light beam LR, and the output becomes zero during the irradiation of the sample measurement light beam LS. Summing amplifier 2
7, the detection signal is added to the detection signal S of the 100% diffused light with respect to the sample measurement light beam LS.
(100) and the detection signal R for the reference light beam LR appear alternately. Therefore, based on this output signal, the arithmetic processing unit 2
8 calculates the ratio D (100) = S (100) / R between the two detection signals.

【0016】次に、測定試料載置位置aに測定対象の未
知試料を置き同様の測定を行なうと、加算アンプ27の
出力信号には試料測定光束LSに対する未知試料の拡散
光の検出信号S(S)と参照光束LRに対する検出信号Rと
が交互に現われる。これにより、演算処理部28は両検
出信号の比D(S)=S(S)/Rを算出し、更にD(100)と
D(S)の比T=D(S)/D(100)=S(S)/S(100)を計算
することにより反射率を算出する。
Next, when an unknown sample to be measured is placed at the measurement sample mounting position a and the same measurement is performed, the output signal of the addition amplifier 27 shows a detection signal S () of diffused light of the unknown sample with respect to the sample measurement light beam LS. S) and the detection signal R for the reference light beam LR appear alternately. As a result, the arithmetic processing unit 28 calculates the ratio D (S) = S (S) / R between the two detection signals, and furthermore, the ratio T = D (S) / D (100) between D (100) and D (S). ) = S (S) / S (100) to calculate the reflectance.

【0017】以上のように、本実施例の分光光度計で
は、参照光束LRが光検出器に到達するまでの光路に積
分球を含んでいないが、反射率等の計算の過程で参照光
束LRに対する検出信号Rの影響はないので、拡散反射
光の捕集効率が高くなる分だけ測定精度が改善される。
但し、例えば、標準白板測定時と未知試料測定時とで周
囲温度が相違しており、試料側光検出器23と参照側光
検出器24との温度依存性の相違が大きいと、反射率の
計算の過程で参照光束LR側の検出信号Rの温度変動分
が影響して精度の低下を招く。従って、試料側光検出器
23と参照側光検出器24とは、できる限り特性の揃っ
たものを用いることが好ましい。
As described above, in the spectrophotometer of the present embodiment, although the light path before the reference light beam LR reaches the photodetector does not include the integrating sphere, the reference light beam LR is calculated in the process of calculating the reflectance and the like. Is not affected by the detection signal R, the measurement accuracy is improved by an increase in the efficiency of collecting diffuse reflected light.
However, for example, when the ambient temperature is different between the measurement of the standard white plate and the measurement of the unknown sample, and the difference in the temperature dependency between the sample-side photodetector 23 and the reference-side photodetector 24 is large, the reflectivity is reduced. In the course of the calculation, the temperature fluctuation of the detection signal R on the side of the reference light beam LR influences and causes a decrease in accuracy. Therefore, it is preferable that the sample-side photodetector 23 and the reference-side photodetector 24 have characteristics as uniform as possible.

【0018】なお、上記実施例では加算アンプ27によ
りアナログ的に両検出信号を加算していたが、それぞれ
A/D変換器によりディジタル信号に変換し、その後に
演算処理を行なって加算又は同等の処理を行なうように
してもよい。
In the above-described embodiment, the two detection signals are added in an analog manner by the addition amplifier 27. However, the two detection signals are converted into digital signals by A / D converters, and thereafter are subjected to arithmetic processing to be added or equivalent. Processing may be performed.

【0019】また、上記実施例は一例であって、本発明
の趣旨の範囲で適宜変形や修正を行なえることは明らか
である。
The above embodiment is merely an example, and it is apparent that modifications and modifications can be made within the spirit of the present invention.

【図面の簡単な説明】[Brief description of the drawings]

【図1】 本発明に係る分光光度計の実施例における積
分球測定部の構成図。
FIG. 1 is a configuration diagram of an integrating sphere measuring unit in an embodiment of a spectrophotometer according to the present invention.

【図2】 従来の分光光度計の積分球測定部の構成図。FIG. 2 is a configuration diagram of an integrating sphere measuring unit of a conventional spectrophotometer.

【符号の説明】[Explanation of symbols]

10…積分球 11…入射窓 12…反射窓 13…光検出窓 23…試料側光検出器 24…参照側光検出器 27…加算アンプ 28…演算処理部 DESCRIPTION OF SYMBOLS 10 ... Integrating sphere 11 ... Incident window 12 ... Reflection window 13 ... Light detection window 23 ... Sample side photodetector 24 ... Reference side photodetector 27 ... Addition amplifier 28 ... Operation processing part

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 試料測定光束及び参照光束を用いるダブ
ルビーム型の分光光度計において、 a)光入射窓から導入した試料測定光を光反射窓の外側近
傍に配置した試料に照射し、該試料からの拡散反射光を
内面に反射させて光検出窓に導くように、光入射窓、光
反射窓及び光検出窓を適宜の位置に開口した積分球と、 b)前記光検出窓を通して積分球の外側に取り出された光
を検出する第1の光検出手段と、 c)前記積分球の外部において参照光束を検出する第2の
光検出手段と、 d)第1及び第2の光検出手段の検出信号を基に、試料の
光学的な特性を示す指標値を算出する演算手段と、 を備えることを特徴とする分光光度計。
1. A double beam type spectrophotometer using a sample measurement light beam and a reference light beam, comprising: a) irradiating a sample arranged in the vicinity of the outside of a light reflection window with a sample measurement light introduced from a light incident window; An integrating sphere in which a light incident window, a light reflecting window and a light detecting window are opened at appropriate positions so as to reflect the diffuse reflected light from the inner surface to the light detecting window, and b) an integrating sphere through the light detecting window. First light detecting means for detecting light taken out of the integrating sphere; c) second light detecting means for detecting a reference light beam outside the integrating sphere; and d) first and second light detecting means. And a calculating means for calculating an index value indicating an optical characteristic of the sample based on the detection signal of (1).
JP8334998A 1996-11-29 1996-11-29 Spectrophotometer Pending JPH10160571A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP8334998A JPH10160571A (en) 1996-11-29 1996-11-29 Spectrophotometer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP8334998A JPH10160571A (en) 1996-11-29 1996-11-29 Spectrophotometer

Publications (1)

Publication Number Publication Date
JPH10160571A true JPH10160571A (en) 1998-06-19

Family

ID=18283596

Family Applications (1)

Application Number Title Priority Date Filing Date
JP8334998A Pending JPH10160571A (en) 1996-11-29 1996-11-29 Spectrophotometer

Country Status (1)

Country Link
JP (1) JPH10160571A (en)

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