JPH03272425A - spectrophotometer - Google Patents

spectrophotometer

Info

Publication number
JPH03272425A
JPH03272425A JP7151890A JP7151890A JPH03272425A JP H03272425 A JPH03272425 A JP H03272425A JP 7151890 A JP7151890 A JP 7151890A JP 7151890 A JP7151890 A JP 7151890A JP H03272425 A JPH03272425 A JP H03272425A
Authority
JP
Japan
Prior art keywords
array sensor
spectral image
peak
image plane
wavelength
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
JP7151890A
Other languages
Japanese (ja)
Inventor
Hideo Hattori
秀雄 服部
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 JP7151890A priority Critical patent/JPH03272425A/en
Publication of JPH03272425A publication Critical patent/JPH03272425A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01JMEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J3/00Spectrometry; Spectrophotometry; Monochromators; Measuring colours
    • G01J3/28Investigating the spectrum
    • G01J3/2803Investigating the spectrum using photoelectric array detector

Landscapes

  • Physics & Mathematics (AREA)
  • Spectroscopy & Molecular Physics (AREA)
  • General Physics & Mathematics (AREA)
  • Photometry And Measurement Of Optical Pulse Characteristics (AREA)
  • Spectrometry And Color Measurement (AREA)

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明はアレー状センサを用いた多波長同時測定型の分
光光度計に関する。
DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to a multi-wavelength simultaneous measurement type spectrophotometer using an array sensor.

(従来の技術) アレー状センサを用いた多波長同時測定型の分光光度計
は波長走査型の分光光度計に比し、測定所要時間が著る
しく短縮される利点がある。反面スペクトル像をアレー
状センサの単位素子の配列ピッチで分割して個々の分割
部分毎に測定を行うことになるため波長分解能を高くす
ることが困難で、例えば可視域だけの測定として波長範
囲400>700nmをカバーする場合、接近した二つ
のピークを識別できるためには二つのピークの間に少く
とも一つの単位素が挟まっていなくてはならないから、
1024単位素子のセンサを用いるとすると、波長分解
能は3001512nmで約0.6nmとなるが、実際
にはピーク中心が二つの単位素子の間の不感光部分に来
るようなこともあって、波長分解能はlnmが限度であ
る。更にピーク中心が単位素子の中央に来た場合と、二
つの単位素子の中間に来た場合とでは測定されるピーク
強度に大きな差が現われ、測定結果が歪んだものとなる
(Prior Art) A multi-wavelength simultaneous measurement type spectrophotometer using an array sensor has the advantage that the time required for measurement is significantly reduced compared to a wavelength scanning type spectrophotometer. On the other hand, since the spectral image is divided by the arrangement pitch of the unit elements of the array sensor and measurement is performed for each divided part, it is difficult to increase the wavelength resolution.For example, when measuring only the visible range, it is difficult to increase the wavelength resolution. When covering >700 nm, at least one unit element must be sandwiched between two peaks in order to distinguish between two peaks that are close to each other.
If a sensor with 1024 unit elements is used, the wavelength resolution will be approximately 0.6 nm at 3001512 nm, but in reality, the peak center may be in the non-light-sensitive area between two unit elements, so the wavelength resolution will be The limit is lnm. Furthermore, there is a large difference in the measured peak intensity between when the peak center is at the center of a unit element and when it is between two unit elements, and the measurement results are distorted.

(発明が解決しようとする課題〉 上述したスペクトルビークの中心が単位素子の中央に来
た場合と単位素子の間の不感光帯に来た場合とで測光出
力が大幅に異ると云う問題は一つのピークが幾つかの単
位素子にまたがるようにすることで解消されるが、その
ようにすると単位波長差に対応させる単位素子数が増し
、波長分解能が一層低くなる。
(Problem to be Solved by the Invention) The above-mentioned problem that the photometric output differs significantly between when the center of the spectral peak is at the center of the unit element and when it is at the dead zone between the unit elements can be solved. This problem can be solved by making one peak span several unit elements, but in this case the number of unit elements corresponding to a unit wavelength difference increases and the wavelength resolution becomes even lower.

本発明はアレー状センサを用いた同時測定型分光光度計
の高速性を失うことなく、波長分解能を上げ、また上述
したスペクトルピークが単位素子配列のどこに位置する
かで測定出力が異ると云う問題を解消しようとするもの
である。
The present invention improves wavelength resolution without sacrificing the high speed of a simultaneous measurement type spectrophotometer using an array sensor, and the measurement output differs depending on where the above-mentioned spectral peak is located in the unit element array. It is an attempt to solve the problem.

(課題を解決するための手段) スペクトル像面上のスペクトル像を波長展開方向に、同
像面上のアレー状センサの単位素子の配列ピッチの複数
分の1を1移動ステップとして上記単位素子の1ピツチ
分だけステップ状に移動させるように、分光器の入口ス
リット或は分光素子を、或は入口スリット、分光素子は
固定でアレー状センサ自身を上述同様複数分の1素子分
ずつピエゾ素子駆動機構で段階的に駆動させると共に、
上記駆動の1ステップの毎の上記アレー状センサの出力
を上記lステップ移動対応量だけずらせて記録するよう
にした。
(Means for Solving the Problem) A spectral image on a spectral image plane is moved in the wavelength expansion direction, with one plurality of the arrangement pitch of the unit elements of the array sensor on the same image plane being taken as one movement step. The entrance slit or the spectroscopic element of the spectrometer is moved stepwise by one pitch, or the entrance slit and the spectroscopic element are fixed and the array sensor itself is driven by the piezo element one element at a time as described above. In addition to being driven in stages by a mechanism,
The output of the array sensor for each step of the drive is recorded with a shift corresponding to the l-step movement.

(作用) 分光器の入口スリット或は分光素子を動かすことにより
、スペクトル像面上でスペクトル像を波長展開方向に移
動させることができる。本発明はこのための入口スリッ
ト或は分光素子の駆動をピエゾ素子駆動機構によって段
階的に行う。段階的駆動はピエゾ素子に印加する電圧を
段階的に変化させればよく、ピエゾ素子は応答速度がき
わめて速く、μSの時間幅でも応答できる。アレー状セ
ンサは例えばフォトダイオードアレーであれば全波長域
の一回の測定所要時間は数10 m sであるから、1
ステップにこの程度の時間をかけての駆動はきわめて容
易である。
(Function) By moving the entrance slit of the spectrometer or the spectroscopic element, the spectral image can be moved in the wavelength expansion direction on the spectral image plane. In the present invention, the entrance slit or the spectroscopic element for this purpose is driven in stages by a piezo element drive mechanism. Stepwise driving can be achieved by changing the voltage applied to the piezo element in steps, and the piezo element has an extremely fast response speed and can respond even in a time width of μS. For example, if the array sensor is a photodiode array, the time required for one measurement over the entire wavelength range is several tens of milliseconds.
It is extremely easy to drive a step that takes this much time.

また本発明ではアレー状センサの単位素子の配列ピッチ
の複数分の−例えば1/4を1ステップとして1ピツチ
分だけスペクトルを移動させるので、各単位素子は単位
素子の1ピツチ間を波長走査して、各ステップ毎に測定
出力をサンプリングするのと同じことになる。例えば1
ピツチの174を1ステップとして3ステップ移動させ
るので、1ステップ毎に数100m5をかけても約0.
4秒で一回の測定を終ることができ、多波長同時分光光
度計の高速性は失われない。
In addition, in the present invention, the spectrum is moved by one pitch, with a plurality of pitches, for example, 1/4, of the arrangement pitch of the unit elements of the array sensor being moved by one pitch, so each unit element scans the wavelength between one pitch of the unit elements. This is equivalent to sampling the measurement output at each step. For example 1
Since we move 3 steps with 174 pitches as one step, even if we multiply several 100 m5 for each step, it will be approximately 0.
A single measurement can be completed in 4 seconds, maintaining the high speed of a multi-wavelength simultaneous spectrophotometer.

更に測定結果は各ステップの測定出力を記録上で1ステ
ップ相当分ずつずらせて記録するので、スペクトル記録
面では、単位素子1ピッチ分の間に各ステップの測定値
が並んで、スペクトル像のサンプリング間隔を単位素子
ピッチ相当分の複数分の1の間隔として一つのスペクト
ル像の記録が得られ、波長分解能かじ向上すると共に、
スペクトルビークの中心が単位素子の中央に来るか単位
素子の間の不感帯に来るかによる測定出力の違いと云っ
た問題も解消される。
Furthermore, the measurement results are recorded by shifting the measurement output of each step by one step on the record, so on the spectrum recording surface, the measurement values of each step are lined up between one pitch of the unit element, and the sampling of the spectral image is performed. One spectral image can be recorded by setting the interval to a multiple of the unit element pitch, and the wavelength resolution is greatly improved.
This also solves the problem of differences in measurement output depending on whether the center of the spectral peak is at the center of the unit element or in the dead zone between the unit elements.

(実施例〉 第1図に本発明の一実施例を示す。図でMは分光器、P
はピエゾ素子駆動機構の駆動電源、Cはデータ処理およ
び装置制御を行う制御装置、Rは表示装置である。分光
器Mにおいて、Gは分光素子である回折格子、Sは入口
スリットで0点を支点とする揺動台B上に取付けられて
おり、揺動台Bの一側面にピエゾ素子駆動機4$1Qの
先端が当接させてあって、同駆動素子の伸縮に応じて入
口スリットSが矢印aの方向に移動せしめられる。Dは
アレー状センサでフォトダイオードアレーが用いられて
おり、この面上にスペクトル像かじ形成され、入口スリ
ットSの上記矢印方向の移動により、アレー状センサ面
上でスペクトル像が矢印す方向に移動する。Lは分光光
度計の光源、Kは集光レンズである。
(Example) Fig. 1 shows an example of the present invention. In the figure, M is a spectrometer, P
is a drive power source for the piezo element drive mechanism, C is a control device that performs data processing and device control, and R is a display device. In the spectrometer M, G is a diffraction grating that is a spectroscopic element, S is an entrance slit, and it is installed on a rocking table B with the 0 point as a fulcrum. The tip of the drive element 1Q is brought into contact with the drive element, and the entrance slit S is moved in the direction of the arrow a according to the expansion and contraction of the drive element. D is an array-like sensor that uses a photodiode array, and a spectral image is formed on this surface, and as the entrance slit S moves in the direction of the arrow above, the spectral image moves on the array-like sensor surface in the direction of the arrow. do. L is the light source of the spectrophotometer, and K is the condenser lens.

次に第2図を用いて上記装置の動作を説明する。第2図
でPはスペクトルの一つのピークを示す。nはアレー状
センサのn番目の単位素子、n+1は同じくn+1番目
の単位素子である。図で点Oは最初スペクトルビークP
の中心があった位置であり、入口スリットSの3ステッ
プの移動によりスペクトルビーク中心の位置は第2図の
点1.2.3と移動し、夫々のステップで、アレー状素
子の全単位素子の出力が制御装置Cに取込まれる。下表
はアレー状センサの単位素子nとn+1の、スペクトル
ビークPK中心位置0.1〜3における出力を示す。
Next, the operation of the above device will be explained using FIG. In FIG. 2, P indicates one peak of the spectrum. n is the n-th unit element of the array sensor, and n+1 is the n+1-th unit element. In the figure, point O is the initial spectral peak P
By moving the entrance slit S in three steps, the center of the spectral peak moves to point 1.2.3 in Fig. 2. At each step, all unit elements of the array element are The output of is taken into control device C. The table below shows the outputs of unit elements n and n+1 of the array sensor at spectral peak PK center positions 0.1 to 3.

表 ピーク位Ml    nの出力   n+1の出力Oビ
ーククの左半分 ピークなし 1     ピークの左裾  ピークの右裾2    
 ピークなし   ピークの右半分3     ピーク
なし   ピーク全体本発明では上の出力を表示装置R
において第3図に示すような形で記録する。この図で各
プロットされた点の符号は(n)、(n+1)で単位素
子を示し、その右の数字でピーク位置O〜3を示す。例
えば(n)Oはピーク中心が第2図O位置にあるときの
単位素子nの出力であり、上記表のn欄の一番上の出力
である。第3図でTがアレー状センサの単位素子の1ピ
ツチに相当し、このlピッチ間を3ステップでスペクト
ルビークが移動しているので、−単位素子につき、この
1ピツチ間に4個の測定出力が得られ、それらの出力を
この1ピツチ間の4点に順次ずらせて記録する。この記
録点をつなぐと第3図の曲線Fのようにピークのプロフ
ァイルが画かれ、アレー状センサの単位素子配列ピッチ
の1/2の幅のピークのプロファイルが4点で測定され
ていることになる。
Table peak position Ml Output of n Output of n+1 Left half of O Beak No peak 1 Left tail of peak Right tail of peak 2
No peak Right half of peak 3 No peak Entire peak In the present invention, the above output is displayed on display device R.
Record it in the form shown in Figure 3. In this figure, the symbols of each plotted point are (n) and (n+1) to indicate the unit element, and the numbers to the right indicate the peak positions O to 3. For example, (n)O is the output of unit element n when the peak center is at position O in FIG. 2, and is the top output in column n of the above table. In Figure 3, T corresponds to 1 pitch of the unit element of the array sensor, and the spectral peak moves in 3 steps between this 1 pitch, so 4 measurements are taken during this 1 pitch for each unit element. Outputs are obtained, and these outputs are sequentially shifted and recorded at four points between this one pitch. When these recorded points are connected, a peak profile is drawn as shown by curve F in Figure 3, and the peak profile with a width of 1/2 of the unit element arrangement pitch of the array sensor is measured at four points. Become.

上述実擁例では人口スリットを分光器波長分散方向に駆
動しているが、ピエゾ駆動機構を用いて分光素子或はア
レー状センサ自体を波長分散方向にアレー状センサの単
位素子の配列ピッチの17nずつステップ状に駆動して
上述と同し記録方法でスペクトルを記録させることも、
本発明に含まれることは云うまでもない。
In the above-mentioned example, the artificial slit is driven in the wavelength dispersion direction of the spectrometer, but a piezo drive mechanism is used to drive the spectroscopic element or the array sensor itself in the wavelength dispersion direction at a pitch of 17n, which is the arrangement pitch of the unit elements of the array sensor. It is also possible to record the spectrum using the same recording method as described above by driving it in steps.
It goes without saying that it is included in the present invention.

(発明の効果) 第2図に示すような位置関係でスペクトルピークが存在
した場合、従来方法ではピークは本来の半分の強度であ
ると測定され、ビーク中心が単位素子nの中央に来たと
きと著しく興なった結果になり、更にピーク中心が単位
素子nとn+1の中間に来たときはピークそのものが検
出されないことになる。このようなことを避けるために
は第2図のピークに対して単位素子3〜4個が対応する
ようにしなければならず、一定個数の単位素子で所定の
波長範囲をカバーしようとすると、波長分解能を落さざ
るを得ないが、本発明では一つのピークが単位素子の半
ピツチをカバーできればよいわけだから、著るしく波長
分解能が向上し、ピークプロファイルも画けて、ピーク
の位置により測定値が変化すると云う問題もなくなる。
(Effect of the invention) When a spectral peak exists in the positional relationship shown in Figure 2, in the conventional method, the peak is measured to have half the original intensity, and when the beak center comes to the center of the unit element n. This results in a remarkable result, and furthermore, when the peak center is located between unit elements n and n+1, the peak itself is not detected. In order to avoid this, it is necessary to have 3 to 4 unit elements correspond to the peak in Figure 2, and if you try to cover a predetermined wavelength range with a certain number of unit elements, the wavelength Although resolution has to be degraded, in the present invention, one peak only needs to cover half the pitch of a unit element, so the wavelength resolution is significantly improved, the peak profile can be defined, and measurements can be made based on the peak position. The problem of changing values is also eliminated.

また入口スリット或は分光素子の駆動にピエゾ素子を用
いているので高速動作が可能である。
Furthermore, since a piezo element is used to drive the entrance slit or the spectroscopic element, high-speed operation is possible.

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

第1図は本発明の一実施例装置の平面図、第2図は本発
明装置の動作説明図、第3図は同じく記録形態の説明図
である。 M・・・分光器、S・・・入口スリット、Q・・・回折
格子、D・・・アレー状センサ、P・・・ピエゾ素子駆
動機構駆動電源、C・・・制御装置、R・・・表示装置
FIG. 1 is a plan view of an apparatus according to an embodiment of the present invention, FIG. 2 is an explanatory diagram of the operation of the apparatus of the present invention, and FIG. 3 is an explanatory diagram of the recording format. M...Spectroscope, S...Entrance slit, Q...Diffraction grating, D...Array sensor, P...Piezo element drive mechanism drive power supply, C...Control device, R...・Display device.

Claims (2)

【特許請求の範囲】[Claims] (1)分光器のスペクトル像面上で波長分散方向にスペ
クトル像を移動させるように可動な入口スリット或は分
散素子と、スペクトル像面上に配置されたアレー状セン
サと、上記入口スリット或は分光素子を駆動するピエゾ
駆動機構と、スペクトル像面上のスペクトルの移動の1
ステップがアレー状センサの単位素子の配列ピッチの1
/n(nは複数)であるように(n−1)ステップだけ
上記入口スリット或は分光素子を駆動するように上記ピ
エゾ駆動機構を制御すると共に、その各ステップ毎のア
レー状センサ出力を波長方向にその1ステップ分ずつず
らせて記録させる制御装置とよりなる分光光度計。
(1) An entrance slit or dispersion element movable so as to move the spectral image in the wavelength dispersion direction on the spectral image plane of the spectrometer, an array-shaped sensor arranged on the spectral image plane, and the entrance slit or The piezo drive mechanism that drives the spectroscopic element and the movement of the spectrum on the spectral image plane.
The step is 1 of the arrangement pitch of the unit element of the array sensor.
The piezo drive mechanism is controlled to drive the entrance slit or spectroscopic element by (n-1) steps so that /n (n is plural), and the output of the array sensor for each step is A spectrophotometer consisting of a control device that records data by shifting the direction one step at a time.
(2)分光器においてスペクトル像面に沿って配置され
たアレー状センサを、上記スペクトル像面に沿って波長
分散方向に駆動するピエゾ駆動機構と、上記アレー状セ
ンサのスペクトル像面に沿う移動の1ステップがアレー
状センサの単位素子の配列ピッチの1/n(nは複数)
であるように(n−1)ステップだけアレー状センサを
駆動するように上述ピエゾ駆動機構を制御すると共に、
その各ステップ毎のアレー状センサ出力を波長方向にそ
の1ステップ分ずつずらせて記録させる制御装置とより
なる分光光度計。
(2) A piezo drive mechanism that drives the array sensor arranged along the spectral image plane in the spectrometer in the wavelength dispersion direction along the spectral image plane, and a piezo drive mechanism that drives the array sensor arranged along the spectral image plane in the spectrometer. One step is 1/n (n is plural) of the arrangement pitch of the unit elements of the array sensor.
The piezo drive mechanism described above is controlled to drive the array sensor by (n-1) steps so that
A spectrophotometer comprising a control device that records the array sensor output for each step by shifting it by one step in the wavelength direction.
JP7151890A 1990-03-20 1990-03-20 spectrophotometer Pending JPH03272425A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP7151890A JPH03272425A (en) 1990-03-20 1990-03-20 spectrophotometer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP7151890A JPH03272425A (en) 1990-03-20 1990-03-20 spectrophotometer

Publications (1)

Publication Number Publication Date
JPH03272425A true JPH03272425A (en) 1991-12-04

Family

ID=13463018

Family Applications (1)

Application Number Title Priority Date Filing Date
JP7151890A Pending JPH03272425A (en) 1990-03-20 1990-03-20 spectrophotometer

Country Status (1)

Country Link
JP (1) JPH03272425A (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE4017317A1 (en) * 1990-05-30 1991-12-05 Bodenseewerk Perkin Elmer Co System for enhancing spectrometer resolution - shifts spectrum periodically relative to detector array
DE19815080C1 (en) * 1998-04-06 1999-09-09 Inst Physikalische Hochtech Ev Spectrometer spectral resolution enhancement device for emission or absorption spectral,analysis
DE19813950C1 (en) * 1998-03-28 1999-11-04 Analytik Jena Gmbh Analysenmes Spectrometer arrangement, pref. for emission and absorption analysis of a specimen using UV-visible spectrometry
FR2810732A1 (en) * 2000-06-27 2001-12-28 Jobin Yvon S A Method for making spectroscopic measurements with higher definition, comprises use of photodetector matrix to make successive recordings after relative displacement between matrix and spectrum

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
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DE4017317C2 (en) * 1990-05-30 2000-02-17 Bodenseewerk Perkin Elmer Co Anode to improve the resolution of a spectrometer
DE19813950C1 (en) * 1998-03-28 1999-11-04 Analytik Jena Gmbh Analysenmes Spectrometer arrangement, pref. for emission and absorption analysis of a specimen using UV-visible spectrometry
DE19815080C1 (en) * 1998-04-06 1999-09-09 Inst Physikalische Hochtech Ev Spectrometer spectral resolution enhancement device for emission or absorption spectral,analysis
FR2810732A1 (en) * 2000-06-27 2001-12-28 Jobin Yvon S A Method for making spectroscopic measurements with higher definition, comprises use of photodetector matrix to make successive recordings after relative displacement between matrix and spectrum

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