JPS63300941A - Zero correcting device for optical measuring instrument - Google Patents
Zero correcting device for optical measuring instrumentInfo
- Publication number
- JPS63300941A JPS63300941A JP13685687A JP13685687A JPS63300941A JP S63300941 A JPS63300941 A JP S63300941A JP 13685687 A JP13685687 A JP 13685687A JP 13685687 A JP13685687 A JP 13685687A JP S63300941 A JPS63300941 A JP S63300941A
- Authority
- JP
- Japan
- Prior art keywords
- optical
- light
- zero
- photoreceptor
- correction
- 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.)
- Granted
Links
- 230000003287 optical effect Effects 0.000 title claims abstract description 50
- 238000012937 correction Methods 0.000 claims abstract description 47
- 230000007246 mechanism Effects 0.000 claims abstract description 17
- 108091008695 photoreceptors Proteins 0.000 claims description 38
- 230000003321 amplification Effects 0.000 claims description 2
- 238000003199 nucleic acid amplification method Methods 0.000 claims description 2
- 239000011521 glass Substances 0.000 abstract description 7
- 238000005259 measurement Methods 0.000 description 15
- 238000000034 method Methods 0.000 description 10
- 238000010586 diagram Methods 0.000 description 4
- 238000001514 detection method Methods 0.000 description 3
- 230000000694 effects Effects 0.000 description 3
- 238000011088 calibration curve Methods 0.000 description 2
- 201000004384 Alopecia Diseases 0.000 description 1
- 238000009825 accumulation Methods 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 238000007689 inspection Methods 0.000 description 1
- WQGWDDDVZFFDIG-UHFFFAOYSA-N pyrogallol Chemical compound OC1=CC=CC(O)=C1O WQGWDDDVZFFDIG-UHFFFAOYSA-N 0.000 description 1
- 239000013589 supplement Substances 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
- G01N21/25—Colour; Spectral properties, i.e. comparison of effect of material on the light at two or more different wavelengths or wavelength bands
- G01N21/27—Colour; Spectral properties, i.e. comparison of effect of material on the light at two or more different wavelengths or wavelength bands using photo-electric detection ; circuits for computing concentration
- G01N21/274—Calibration, base line adjustment, drift correction
Landscapes
- Physics & Mathematics (AREA)
- Engineering & Computer Science (AREA)
- Mathematical Physics (AREA)
- Theoretical Computer Science (AREA)
- Spectroscopy & Molecular Physics (AREA)
- Health & Medical Sciences (AREA)
- Life Sciences & Earth Sciences (AREA)
- Chemical & Material Sciences (AREA)
- Analytical Chemistry (AREA)
- Biochemistry (AREA)
- General Health & Medical Sciences (AREA)
- General Physics & Mathematics (AREA)
- Immunology (AREA)
- Pathology (AREA)
- Spectrometry And Color Measurement (AREA)
- Investigating Or Analysing Materials By Optical Means (AREA)
- Photometry And Measurement Of Optical Pulse Characteristics (AREA)
Abstract
Description
【発明の詳細な説明】
〈産業上の利用分野〉
本発明は、示差屈折計や分光光度51等各種光学測定器
における1口補正装置に関するものである。DETAILED DESCRIPTION OF THE INVENTION <Industrial Application Field> The present invention relates to a one-port correction device for various optical measuring instruments such as a differential refractometer and a spectrophotometer 51.
即ち、光学測定器における検出機構の多くは、測定開始
前の光のエネルギーレベルと測定時における光のエネル
ギーレベルとの差を電気信号に変換する方式になってい
る。従ってこの場合、当然のことながら測定開始前にお
ける出力がゼ[1を表示するように設定しておく必要が
あり、この出力をゼロに設定するための機構をゼロ補正
機構(装置)と言う。That is, most of the detection mechanisms in optical measuring instruments are of a type that converts the difference between the energy level of light before starting measurement and the energy level of light during measurement into an electrical signal. Therefore, in this case, it is of course necessary to set the output to display ze[1 before starting the measurement, and the mechanism for setting this output to zero is called a zero correction mechanism (device).
〈従来の技術〉
この種ぜ口補正を自動的に行なう機構には、受光体に入
射する光を光学補iF、 B11構でコントロール1゛
る光学的オートゼロ方式と、測定開始前の誤差電圧に相
当する電圧を外部から与えて相殺する電気的オートゼロ
方式とがある。光学的オートゼロ方式は光のエネルギー
を測定開始前に常に同一とすることが出来るためエネル
ギーレベルの変動に伴なう測定時の試料濃度と出力との
関係を示す検問線の直線性及び直線性の範囲が常に一定
どなる利点を有するが、受光体に入射する光学や光軸を
調整するための光学補正B!横を制御モータで駆動2き
Uなければならない為、ゼロ補正4業に時間が掛り、速
く駆動させるとぜ口補正のM麿が低下すると言った不具
合がある。又、電気的オートゼロ方式ではげ0補正時間
は速いが光学的エネルギーレベルのバランス補正を行な
わない為、倹伍線の変動を伴ない測定値の補正を必要と
する不具合がある。<Prior art> The mechanism for automatically performing this type of edge correction includes an optical auto-zero method in which the light incident on the photoreceptor is controlled by an optical compensation iF and B11 structure, and an optical auto-zero method that controls the light incident on the photoreceptor by adjusting the error voltage before starting the measurement. There is an electrical auto-zero method in which a corresponding voltage is applied externally to cancel it out. Since the optical auto-zero method can always keep the light energy the same before starting measurement, it is possible to improve the linearity of the check line that shows the relationship between sample concentration and output during measurement due to fluctuations in energy level. It has the advantage that the range is always constant, but optical correction B for adjusting the optical axis and optical axis incident on the photoreceptor! Since the side must be driven by a control motor, it takes time to perform the zero correction, and if the drive is made faster, there is a problem in that the M range of the gap correction decreases. Further, although the electrical auto-zero method has a fast zero-baldness correction time, it does not perform balance correction of the optical energy level, so there is a problem in that the measurement value is required to be corrected due to fluctuations in the margin line.
〈発明が解決しようとする問題点〉
本発明はこの様な従来の不具合に鑑みてなされたもので
あり、ゼロ補正に要する時間を従来の光学的オートゼロ
方式よりも大巾に短縮させることが出来ると共に、ゼロ
補正の精度を従来の光学的オートゼロ方式と同程度とす
ることが出来、しかも光学的エネルギーレベルのバラン
スを測定開始前に常に同一となし検量線の直線性及び直
線性の範囲を常に一定に保持することが出来る光学測定
器におけるゼロ補正装置を提供せんとするものである。<Problems to be Solved by the Invention> The present invention has been made in view of these conventional problems, and can significantly reduce the time required for zero correction compared to the conventional optical auto-zero method. At the same time, the accuracy of zero correction can be made to be on the same level as the conventional optical auto-zero method, and the optical energy level balance is always the same before starting measurement, and the linearity and linearity range of the calibration curve are always maintained. It is an object of the present invention to provide a zero correction device for an optical measuring instrument that can be maintained constant.
く問題点を解決するための手段〉
係る目的を達成する本発明光学測定器におけるゼロ補正
装置は受光体に入射する光をコントロールする光学補正
機構の制御回路を上記受光体と電気的に接続さぜると共
に、受光体出力増巾回路の出力側に電気的ゼロ補正回路
を接続させた事を特徴としたものである。Means for Solving the Problems〉 The zero correction device in the optical measuring instrument of the present invention that achieves the above object has a control circuit for an optical correction mechanism that controls the light incident on the photoreceptor, which is electrically connected to the photoreceptor. In addition, an electrical zero correction circuit is connected to the output side of the photoreceptor output amplification circuit.
〈実施例〉
以下、本発明実施例を図面に基づいて説明する3゜第1
図は示差屈折計の例を示し、第3図は分光光重訂の例を
示すが、この他にも測定開始前の光のエネルギーレベル
と測定時における光のエネルギーレベルとの差を電気信
号に変換する検出機構を備えたあらゆる光学測定器に本
発明装置が適用できることは以下の説明によって容易に
理解されるだろう。<Example> Hereinafter, Example 3 of the present invention will be explained based on the drawings.
The figure shows an example of a differential refractometer, and Fig. 3 shows an example of spectroscopic light revision. It will be easily understood from the following description that the device of the present invention can be applied to any optical measuring instrument equipped with a detection mechanism that converts
第1図において図中1は光源ランプであり、この光源ラ
ンプ1からの光Pは試料セル2を通り、試料ヒル2の後
方に設置した反射鏡3で反射されてガラス板4を通しC
受光体5に入射する。受光体5に入射した光エネルギー
はその受光体5で電気エネルギーに変換され、制御回路
6で増巾されて電気的ゼロ補正回路7に出力される。こ
の反射鏡3から受光体5に至る光学系において、制御回
路6からの信号によって制御モータ8を駆動させガラス
板4の角度を動かすことにより受光体5に入射する光軸
を平行に移動させて、測定開始前の光学的ゼロ補正を行
なうものである。即ち、受光体5に入射する光P+をコ
ントロールする光学補正機構は、ガラス板4とそのガラ
ス板4を動かすための制御モータ8及び制御モータ8を
駆動させる制御回路6とで構成され、その制御回路7を
受光体5と電気的に接続させてなり、測定開始前の状態
において試料側受光素子と対照側受光素子からなる受光
体5に入射した光P+が上記試料側受光素子と対照側受
光素子とに均等に入射されていない場合には、受光体5
からそれに応じた信号が出力されて制御回路6に印加さ
れ、その信号によって試料側受光素子と対照側受光素子
とに光が均等に入射するように制御モータ8を介してガ
ラス板4が動かされ、受光体5に入射する光軸を平行に
移動させて光学的ゼロ補正を行なうものである。In FIG. 1, 1 is a light source lamp, and light P from this light source lamp 1 passes through a sample cell 2, is reflected by a reflecting mirror 3 installed behind the sample hill 2, passes through a glass plate 4, and then passes through a C.
The light enters the photoreceptor 5. The light energy incident on the photoreceptor 5 is converted into electrical energy by the photoreceptor 5, amplified by the control circuit 6, and output to the electrical zero correction circuit 7. In the optical system from the reflector 3 to the photoreceptor 5, the control motor 8 is driven by a signal from the control circuit 6 to move the angle of the glass plate 4, thereby moving the optical axis incident on the photoreceptor 5 in parallel. , performs optical zero correction before starting measurement. That is, the optical correction mechanism that controls the light P+ incident on the photoreceptor 5 is composed of a glass plate 4, a control motor 8 for moving the glass plate 4, and a control circuit 6 for driving the control motor 8. The circuit 7 is electrically connected to the photoreceptor 5, and the light P+ incident on the photoreceptor 5 consisting of the sample-side photoreceptor and the control-side photoreceptor in the state before the start of measurement is received by the sample-side photoreceptor and the control-side photoreceptor. If the light is not evenly incident on the photoreceptor 5,
A corresponding signal is outputted from the control circuit 6 and applied to the control circuit 6, and the glass plate 4 is moved by the control motor 8 so that the light is evenly incident on the sample-side light-receiving element and the control-side light-receiving element. , optical zero correction is performed by moving the optical axis incident on the photoreceptor 5 in parallel.
次いで、制御回路6の出力側に電気的ゼロ補正回路7を
接続させて、電気的ゼロ補正を行なう。Next, an electrical zero correction circuit 7 is connected to the output side of the control circuit 6 to perform electrical zero correction.
この電気的ゼロ補正回路7は測定開始前の誤差電圧に相
当する電圧を外部から与えて相殺する回路となっ゛てお
り、τ1体的には第2図に示す如く基本的に、受光体5
から人力される電圧の大小(プラス・マイナス)を判別
するためのコンパレータ20と、そのコンパレータ20
の判別にしたがい電圧の加減算を行なうアップダウンカ
ウンタ21と、誤差電圧を相殺する為の差動増巾器22
とで構成される。This electrical zero correction circuit 7 is a circuit that applies a voltage corresponding to the error voltage before the start of measurement from the outside to cancel it out. Basically, as shown in FIG.
A comparator 20 for determining the magnitude (plus/minus) of the voltage manually applied from the
an up/down counter 21 that adds or subtracts voltage according to the determination of
It consists of
然して、測定開始前の状態において受光体5に入射した
光P1が試料側受光素子と対照側受光素子とに均等に入
射されていない場合には、受光体5からそれに応じた信
号が出力されるので、その信号を差動増巾器22の一方
の入力端子23から入力さけ、その出力をコンパレータ
20に入力させる。コンパレータ20では入力された信
号の電圧の差をL口Vに対してIIIGII側にあるか
[〇−側にあるかを比較判別し、その判別結果にしたが
いアップダウンカウンタ21でもって旧Gllの時は加
算を行ないシ〇−の時は減算を行ない、+INと−IN
の入力がバランスしたところでアップダウンカウンタ2
1はバランスし平衡状態を保持し、差動増巾器22に出
力する。However, if the light P1 incident on the photoreceptor 5 is not equally incident on the sample-side light-receiving element and the control-side photoreceptor in the state before the start of measurement, the photoreceptor 5 outputs a corresponding signal. Therefore, the signal is not inputted from one input terminal 23 of the differential amplifier 22, and its output is inputted to the comparator 20. The comparator 20 compares and determines whether the voltage difference of the input signal is on the IIIGII side or the [○- side with respect to the L port V, and according to the result of the determination, the up/down counter 21 is used to determine whether it is on the old Gll side. performs addition, and when it is ○-, it performs subtraction, +IN and -IN
When the inputs of are balanced, up/down counter 2
1 is balanced, maintains an equilibrium state, and outputs it to the differential amplifier 22.
このアップダウンカウンタ21が平衡状態の時にラッチ
をかけると、その出力電圧はこのILlの電圧をラッチ
が解かれるまで、入力電圧が変化してもこの電圧を保持
し続ける。これで電気的ゼロ補正が行なわれる。If this up/down counter 21 is latched when it is in a balanced state, its output voltage will continue to hold the voltage of IL1 even if the input voltage changes until the latch is released. Electrical zero correction is now performed.
又、第3図は分光光度計の例を示し、図中9は入射して
来た光Pを試料側受光体5aと対照側受光体5bとに振
り分けるためのハーフミラ−であり、10a 、 10
bは受光体5a、 5bに入射する光♀を調整するため
の絞り(スリット)であり、図中第1図と同じ符号は同
様の構成部材を示す。この例では受光体5a、 5bに
入射する光Pをコントロールする光学補正機構は、ハー
フミラ−9とそのハーフミラ−9を動かすための制御モ
ータ8及び制御モータ8を駆動させる制御回路6とで構
成される。即ち、測定開始前の状態において試料側受光
体5aと対照側受光体5bとに入射される光量が均等で
ない場合には、それに応じた信号が1.11111回路
6に出力されて試料側受光体5aと対照側受光体5bと
に入射される光のエネルギー(光量)が均等となるよう
に制御モータ8を介してハーフミラ−9の反射角度を変
えて光学的ゼロ補正を行なうものである。Further, FIG. 3 shows an example of a spectrophotometer, in which 9 is a half mirror for distributing the incident light P into a sample-side photoreceptor 5a and a control-side photoreceptor 5b, 10a, 10.
b is a diaphragm (slit) for adjusting the light incident on the photoreceptors 5a and 5b, and the same reference numerals as in FIG. 1 indicate the same components. In this example, the optical correction mechanism that controls the light P incident on the photoreceptors 5a and 5b is composed of a half mirror 9, a control motor 8 for moving the half mirror 9, and a control circuit 6 for driving the control motor 8. Ru. That is, if the amount of light incident on the sample-side photoreceptor 5a and the control-side photoreceptor 5b is not equal in the state before the start of measurement, a corresponding signal is output to the 1.11111 circuit 6 to the sample-side photoreceptor 5b. Optical zero correction is performed by changing the reflection angle of the half mirror 9 via the control motor 8 so that the energy (light amount) of the light incident on the photoreceptor 5a and the contrast side photoreceptor 5b becomes equal.
尚、対照側受光体51)を必要としない単一受光体を使
用した場合でも、試料セル2に達する光I11を同様に
変化させる事により光学的ゼロ補正を行なうことが出来
る。そして、制御回路6の出力は先に説明した電気的ぜ
口補正回路7を通して出力される。Note that even when using a single photoreceptor that does not require the contrasting photoreceptor 51), optical zero correction can be performed by similarly changing the light I11 that reaches the sample cell 2. The output of the control circuit 6 is then outputted through the electrical mouth correction circuit 7 described above.
〈発明の効果〉
本発明光学測定器におけるピロ補正¥7装置は斯様に構
成したので、測定開始前のゼロ補ロー操作を行なうと、
光学補正機構(光学的オートゼロ機構)と電気的ゼロ補
正回路(電気的オーl〜ゼ[1機構)とが連動してはた
らき、従って光学的バランスをとりつつ電気的ゼロ補正
を行なうことが出来、光学的アンバランスによって生じ
る出力の大ぎさのずれを生じることなく迅速に且つ正確
にぜ口補正を行なうことが出来る。即ち、光学的補正機
構は検品線の変化が生じない範囲内に光学バランスを戻
すためにのみはたらかせるので、精度を上げるための速
度制限が大巾に緩和され、結果としてゼロ補正に要する
時間を従来の光学的オートゼロ方式よりも大巾に短縮さ
せることが出来る18又、電気的ゼロの補正範囲を光学
的ゼロの補正範囲内に制限することが出来るので、ゼロ
補正の精度を従来の光学的オートゼロ方式と同程度に保
持することができるものである。<Effects of the Invention> Since the pyro correction ¥7 device in the optical measuring instrument of the present invention is configured in this manner, when performing the zero supplement low operation before starting measurement,
The optical correction mechanism (optical auto-zero mechanism) and the electrical zero correction circuit (electrical auto-zero [1 mechanism) work together, so it is possible to perform electrical zero correction while maintaining optical balance. The gap can be corrected quickly and accurately without causing large deviations in output caused by optical imbalance. In other words, since the optical correction mechanism works only to return the optical balance to a range where no change in the inspection line occurs, the speed limit for increasing accuracy is greatly relaxed, and as a result, the time required for zero correction is reduced. This can be significantly shortened compared to the conventional optical auto-zero method.18 Also, since the electrical zero correction range can be limited to the optical zero correction range, the zero correction accuracy can be improved compared to the conventional optical auto-zero method. It is possible to maintain the same level as the auto-zero method.
しかも、基本的なゼロ補正を光学補正機構(光学的オー
トゼロ機構)で行なっているので、光学的エネルギーレ
ベルのバランスを測定開始前に常に同一となし検出線の
直線性及び直線性の範囲を常に一定に保持することが出
来、繰り返し補正の累積による光学的バランスの不良が
もたらす検量線の変化を来たす虞れがなくなる。第4図
はこの効果を示したグラフであり、tIX軸に出力の大
きさを示し、横軸に光学的バランスのずれの大きさを示
し、光学的バランスの不良によって生じる試料濃度によ
って得られる出力信号の大きさの変化がない事が理解さ
れる。Moreover, since the basic zero correction is performed by an optical correction mechanism (optical auto-zero mechanism), the optical energy level balance is always the same before starting measurement, and the linearity and linearity range of the detection line are always maintained. It can be held constant, and there is no possibility that the calibration curve will change due to poor optical balance due to accumulation of repeated corrections. Figure 4 is a graph showing this effect. The tIX axis shows the magnitude of the output, the horizontal axis shows the magnitude of the deviation in optical balance, and the output obtained by the sample concentration caused by poor optical balance. It can be seen that there is no change in the signal magnitude.
J:って所期の目的を達成し得るJ: Is it possible to achieve the intended purpose?
第1図は本発明第1実施例を示す模式図、第2図は本発
明に係る電気的ぜ口補正回路の実施の一例を示す回路図
、第3図は本発明第2図実施例を示す模式図、第4図は
本発明装置の効果を説明するグラフである。
図中、5.5a、 5bは受光体、6は制御回路、7は
電気的ゼロ補正回路、である。
特許出願人 株式会社 エルマ
/゛′
代 理 人 早 川
政 \ 名 7パ′と−・FIG. 1 is a schematic diagram showing the first embodiment of the present invention, FIG. 2 is a circuit diagram showing an example of implementation of the electrical gap correction circuit according to the present invention, and FIG. 3 is a schematic diagram showing the embodiment of the present invention shown in FIG. The schematic diagram shown in FIG. 4 is a graph explaining the effect of the device of the present invention. In the figure, 5.5a and 5b are photoreceptors, 6 is a control circuit, and 7 is an electrical zero correction circuit. Patent applicant Elma Co., Ltd./゛′ Agent Hayakawa
Government \ Name 7pa' and-・
Claims (1)
制御回路を上記受光体と電気的に接続させると共に、受
光体出力増巾回路の出力側に電気的ゼロ補正回路を接続
させた事を特徴とする光学測定器におけるゼロ補正装置
。A control circuit for an optical correction mechanism that controls light incident on the photoreceptor is electrically connected to the photoreceptor, and an electrical zero correction circuit is connected to the output side of the photoreceptor output amplification circuit. Zero correction device for optical measuring instruments.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62136856A JPH0625735B2 (en) | 1987-05-30 | 1987-05-30 | Zero correction device in optical measuring instrument |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62136856A JPH0625735B2 (en) | 1987-05-30 | 1987-05-30 | Zero correction device in optical measuring instrument |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS63300941A true JPS63300941A (en) | 1988-12-08 |
| JPH0625735B2 JPH0625735B2 (en) | 1994-04-06 |
Family
ID=15185110
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP62136856A Expired - Fee Related JPH0625735B2 (en) | 1987-05-30 | 1987-05-30 | Zero correction device in optical measuring instrument |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0625735B2 (en) |
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH03162651A (en) * | 1989-11-20 | 1991-07-12 | Shimadzu Corp | Polarization type differential refractometer |
| WO2006025104A1 (en) * | 2004-08-31 | 2006-03-09 | Gl Sciences Incorporated | Optical detection method and optical detector |
| JP2008268233A (en) * | 2008-07-30 | 2008-11-06 | Shimadzu Corp | Differential refractive index detector |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| FR2883971B1 (en) * | 2005-03-31 | 2007-11-16 | C2 Diagnostics Sa | OPTICAL BLOOD ANALYSIS DEVICE, ANALYZING APPARATUS EQUIPPED WITH SUCH A DEVICE |
Citations (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5198090A (en) * | 1975-02-26 | 1976-08-28 | Atsuenyuno yubunnodosokuteihoho |
-
1987
- 1987-05-30 JP JP62136856A patent/JPH0625735B2/en not_active Expired - Fee Related
Patent Citations (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5198090A (en) * | 1975-02-26 | 1976-08-28 | Atsuenyuno yubunnodosokuteihoho |
Cited By (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH03162651A (en) * | 1989-11-20 | 1991-07-12 | Shimadzu Corp | Polarization type differential refractometer |
| WO2006025104A1 (en) * | 2004-08-31 | 2006-03-09 | Gl Sciences Incorporated | Optical detection method and optical detector |
| JPWO2006025104A1 (en) * | 2004-08-31 | 2008-05-08 | ジーエルサイエンス株式会社 | Optical detection method and optical detector |
| JP4584254B2 (en) * | 2004-08-31 | 2010-11-17 | ジーエルサイエンス株式会社 | Optical detection method and optical detector |
| JP2008268233A (en) * | 2008-07-30 | 2008-11-06 | Shimadzu Corp | Differential refractive index detector |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0625735B2 (en) | 1994-04-06 |
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