JPS6344189B2 - - Google Patents

Info

Publication number
JPS6344189B2
JPS6344189B2 JP17302782A JP17302782A JPS6344189B2 JP S6344189 B2 JPS6344189 B2 JP S6344189B2 JP 17302782 A JP17302782 A JP 17302782A JP 17302782 A JP17302782 A JP 17302782A JP S6344189 B2 JPS6344189 B2 JP S6344189B2
Authority
JP
Japan
Prior art keywords
image
solid
light
face
detectors
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.)
Expired
Application number
JP17302782A
Other languages
Japanese (ja)
Other versions
JPS5961753A (en
Inventor
Shojiro Hashizume
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 JP17302782A priority Critical patent/JPS5961753A/en
Publication of JPS5961753A publication Critical patent/JPS5961753A/en
Publication of JPS6344189B2 publication Critical patent/JPS6344189B2/ja
Granted 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
    • G01J3/42Absorption spectrometry; Double beam spectrometry; Flicker spectrometry; Reflection spectrometry
    • G01J3/427Dual wavelengths spectrometry
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N21/00Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
    • G01N21/17Systems in which incident light is modified in accordance with the properties of the material investigated
    • G01N21/25Colour; Spectral properties, i.e. comparison of effect of material on the light at two or more different wavelengths or wavelength bands
    • G01N21/31Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry
    • G01N21/314Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry with comparison of measurements at specific and non-specific wavelengths

Landscapes

  • Physics & Mathematics (AREA)
  • Spectroscopy & Molecular Physics (AREA)
  • General Physics & Mathematics (AREA)
  • Health & Medical Sciences (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Chemical & Material Sciences (AREA)
  • Analytical Chemistry (AREA)
  • Biochemistry (AREA)
  • General Health & Medical Sciences (AREA)
  • Immunology (AREA)
  • Pathology (AREA)
  • Spectrometry And Color Measurement (AREA)
  • Investigating Or Analysing Materials By Optical Means (AREA)

Description

【発明の詳細な説明】 本発明は濃度計、特に固体イメージセンサー
(検出器)と分光器とを組み合わせた濃度計に関
するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a densitometer, and particularly to a densitometer that combines a solid-state image sensor (detector) and a spectrometer.

固体イメージ検出器としては、例えばフオトダ
イオードアレイ等が開発されているが、これらは
受光素子が微小であること、これらの受光素子を
直線上、または面状に配列できること、応答が早
いこと等の特徴を有し、分光器と組み合わせて濃
度計の検出器として利用されている。
For example, photodiode arrays have been developed as solid-state image detectors, but these have several advantages, such as the small size of the light-receiving elements, the ability to arrange the light-receiving elements in a straight line or in a plane, and the fast response. It has unique characteristics and is used as a densitometer detector in combination with a spectrometer.

第1図は、この固体イメージ検出器を使用した
周知の二波長測定を行なうように構成した濃度計
の概略図で、図において1は白色光源、2は集光
レンズ、3は被測定試料、例えばTLCプレート
4上に展開された試料スポツトで、集光レンズ2
が光源1からの光をスポツト3上に集光照射す
る。なお、図では光源1は透過用として配置され
ているが、反射用光源(図示省略)を代替的に、
または択一的使用のために付加的に配備してもよ
い。
FIG. 1 is a schematic diagram of a densitometer configured to perform well-known two-wavelength measurement using this solid-state image detector. In the figure, 1 is a white light source, 2 is a condensing lens, 3 is a sample to be measured, For example, at the sample spot developed on the TLC plate 4, the condenser lens 2
focuses the light from the light source 1 onto the spot 3. Note that in the figure, the light source 1 is arranged for transmission, but a reflection light source (not shown) may be used instead.
Or it may be additionally provided for alternative use.

試料スポツト3からの透過光または反射光は、
結像レンズ5によつて分光器の入口スリツト6上
にスポツト3の像3′として結像される。そして
このスポツトの像3′の測定対象部分の光は入口
スリツト6から分光素子(例えば凹面回折格子)
7に入射し分光される。
The transmitted light or reflected light from sample spot 3 is
The spot 3 is imaged by the imaging lens 5 onto the entrance slit 6 of the spectrometer as an image 3'. The light from the measurement target portion of the spot image 3' is transmitted from the entrance slit 6 to a spectroscopic element (for example, a concave diffraction grating).
7 and is separated into spectra.

この回折格子7によつて分光された各波長に対
応するスリツト像6′はスペクトル像面8上に連
続的に形成されるのでこの面8上の適当な位置に
検出器を配置することにより、任意の波長での測
光を行なうことができる。
Slit images 6' corresponding to each wavelength separated by this diffraction grating 7 are continuously formed on the spectral image plane 8, so by placing the detector at an appropriate position on this plane 8, Photometry can be performed at any wavelength.

この場合、二波長測光を行なうには例えば二つ
の検出器9λ1,9λ2をスペクトル像面8上の所望
の波長位置にそれぞれ配置し、また二波長の選択
を行なうには各検出器をスペクトル像面8上で波
長分散方向(横方向)に変位させればよい(なお
検出器の変位と回折格子の回動との組み合わせに
よつても可能である)。
In this case, to perform two-wavelength photometry, for example, two detectors 9λ 1 and 9λ 2 are placed at desired wavelength positions on the spectral image plane 8, and to select two wavelengths, each detector is placed on the spectral image plane 8. It is only necessary to displace it in the wavelength dispersion direction (lateral direction) on the image plane 8 (this is also possible by a combination of detector displacement and rotation of the diffraction grating).

なお、検出器での測定値の以後の処理について
は、二波長測定は周知であるので、説明は省略す
る。
Note that the subsequent processing of the measured values by the detector will not be described since dual wavelength measurement is well known.

上記のような構成においては、次のような問題
点が発生する。すなわち、固体イメージ検出器に
は、これを構成する多数の素子、例えばフオトダ
イオードアレイに接続される配線束が付いている
ので、波長選択のために検出器の位置を変えるご
とに配線束をひきずることになり、断線などの事
故が起り易い。
In the above configuration, the following problems occur. In other words, a solid-state image detector has a wiring bundle connected to the many elements that make up the detector, such as a photodiode array, so the wiring bundle is dragged each time the detector position is changed for wavelength selection. As a result, accidents such as wire breakage are likely to occur.

また、検出器の物理的な大きさによる制限のた
めに、一定間隔よりも接近した二波長位置に二つ
の検出器を並置することができず、波長の自由な
選択は不可能である。
Further, due to limitations due to the physical size of the detectors, it is not possible to arrange two detectors in parallel at two wavelength positions closer than a certain interval, and free selection of wavelengths is not possible.

本発明は以上の欠点を克服するために、スリツ
ト形の入射および出射端面ないしイメージガイド
面をそれぞれ有する少なくとも一対のオプチカル
フアイバーの入射端面を、上記スペクトル像面に
おいて波長分散方向に変位自在に配置するととも
に、上記の出射端面を固定配置された少なくとも
一対の固体イメージ検出器のそれぞれの受光面に
対向配置したものである。
In order to overcome the above drawbacks, the present invention arranges the entrance end faces of at least a pair of optical fibers each having a slit-shaped entrance and exit end face or image guide surface so as to be freely displaceable in the wavelength dispersion direction on the spectral image plane. In addition, the above-mentioned output end face is arranged to face each light receiving surface of at least a pair of fixedly arranged solid-state image detectors.

以下、第2図にしたがつて本発明の実施例を説
明するが、第2図において第1図と同一の参照記
号は第1図と同一の対応する要素を示すので説明
は省略する。
Hereinafter, an embodiment of the present invention will be described with reference to FIG. 2. In FIG. 2, the same reference symbols as in FIG. 1 indicate the same corresponding elements as in FIG. 1, so the explanation will be omitted.

本発明によれば、固体イメージ検出器9λ1,9
λ2はスペクトル像面8上に配置されないで、装置
の適当な位置に固定配置される。10λ1,10λ2
はイメージガイド形オプチカルフアイバーで、そ
れぞれ幅の狭いスリツト形の入射端面(イメージ
ガイド面)Iλ1,Iλ2と出射端面Eλ1,Eλ2とを有
する。
According to the invention, the solid-state image detectors 9λ 1 , 9
λ 2 is not placed on the spectral image plane 8 but is fixedly placed at a suitable position in the device. 10λ 1 , 10λ 2
are image guide type optical fibers each having a narrow slit-shaped entrance end face (image guide face) Iλ 1 , Iλ 2 and an exit end face Eλ 1 , Eλ 2 .

入射端面Iλ1,Iλ2は、それぞれ上述のスリツト
像6′の高さ、幅にほぼ一致しており、スペクト
ル像面8上において各別に波長分散方向に変位可
能に並置されており、一方出射端面Eλ1,Eλ2
それぞれ検出器9λ1,9λ2の受光面に対向配置さ
れている。
The incident end surfaces Iλ 1 and Iλ 2 almost match the height and width of the above-mentioned slit image 6', respectively, and are juxtaposed on the spectral image plane 8 so that they can each be displaced in the wavelength dispersion direction, while the exit end surfaces The end surfaces Eλ 1 and Eλ 2 are arranged to face the light receiving surfaces of the detectors 9λ 1 and 9λ 2 , respectively.

従つて、入射端面Iλ1,Iλ2をそれぞれスペクト
ル像面8上の所望の波長λ1,λ2の位置に配置する
ことにより、その波長の光を検出器9λ1,9λ2
導びくことができる。
Therefore, by arranging the incident end surfaces Iλ 1 and Iλ 2 at the positions of the desired wavelengths λ 1 and λ 2 on the spectral image plane 8, respectively, light of the desired wavelengths can be guided to the detectors 9λ 1 and 9λ 2 . Can be done.

この場合、スペクトル像面8上の像を歪ませる
ことなく検出器9λ1,9λ2の受光面上に投影する
必要があり、このため上記のイメージガイド形オ
プチカルフアイバー10λ1,10λ2はそれぞれの
入射端面Iλ1,Iλ2と出射端面Eλ1,Eλ2において
このオプチカルフアイバーを構成する各フアイバ
ー(素線)が両端面において対応した幾何学的に
同一位置を占めるように配列されていることが必
要である。
In this case, it is necessary to project the image on the spectral image plane 8 onto the light-receiving surfaces of the detectors 9λ 1 and 9λ 2 without distorting it, and for this reason, the above-mentioned image guide type optical fibers 10λ 1 and 10λ 2 are It is noted that the fibers (strands) constituting this optical fiber are arranged at the incident end faces Iλ 1 , Iλ 2 and the exit end faces Eλ 1 , Eλ 2 so as to occupy the same corresponding geometric positions on both end faces. is necessary.

ついで検出器9λ1,9λ2の出力は増幅され測定
目的に応じた適当な回路ないし装置によつて処理
される。
The outputs of the detectors 9λ 1 and 9λ 2 are then amplified and processed by a suitable circuit or device depending on the purpose of measurement.

以上のように、本発明はイメージガイド形オプ
チカルフアイバーのスリツト形入射端面を試料の
透過光または反射光のスペクトル像面上に変位可
能に配備したものであるが、入射端面の幅は固体
イメージ検出器の幅に比べて狭くすることができ
るので、固体イメージ検出器の受光面を直接にス
ペクトル像面上に配置する場合よりもより接近し
た二波長の選択が可能となり分析対象としての試
料の選択性等が広くなる。
As described above, in the present invention, the slit-shaped entrance end face of an image guide type optical fiber is disposed so as to be displaceable on the spectral image plane of the transmitted light or reflected light of the sample. Since it can be narrower than the width of the detector, it is possible to select two wavelengths closer to each other than when the light-receiving surface of the solid-state image detector is placed directly on the spectral image plane, making it easier to select the sample for analysis. Gender etc. become wider.

また、固体イメージ検出器自体を可動とした構
成にともなう断線の危険性等の不都合も排除する
ことができる。
Further, it is also possible to eliminate inconveniences such as the risk of wire breakage due to the configuration in which the solid-state image detector itself is movable.

なお、一般的に試料スポツトには濃度むらがあ
るため、スリツト像の全体を積分したのち吸光度
変換して試料濃度を算出すると測定誤差を生ずる
ことは周知のことである。しかしながら本発明で
は、試料スポツトに濃度むらがあつても、試料ス
ポツトの一部を入口スリツトを通してスペクトル
像に形成し、スペクトル像の相対的強度分布をそ
のままイメージガイド形オプチカルフアイバーで
小さな検出素子をスリツトの長さ方向に並べた例
えばフオトダイオードアレイのような固体イメー
ジ検出器に導びく方式をとつているので、試料ス
ポツトのスペクトル像は測定誤差が無視し得る程
度に細分され、よつて各検出器からの出力が吸光
度変換された後に積分すれば正確な測定ができる
こととなる。
It is well known that a sample spot generally has density unevenness, so that a measurement error will occur if the sample concentration is calculated by integrating the entire slit image and then converting the absorbance. However, in the present invention, even if there is density unevenness in the sample spot, a part of the sample spot is passed through the entrance slit to form a spectral image, and the relative intensity distribution of the spectral image is directly passed through the slit to a small detection element using an image-guided optical fiber. The spectral image of the sample spot is subdivided to the extent that the measurement error is negligible, and each detector Accurate measurements can be made by integrating the output after absorbance conversion.

また上記の実施例においては、二波長測光につ
いて説明したが、これに限らず検出器およびイメ
ージガイド形オプチカルフアイバーを多数設けて
おき、これらのうちの適当な検出器とイメージガ
イド形オプチカルフアイバーの組合わせを利用す
ることにより測光方式の幅広い選択も可能とな
る。
Further, in the above embodiment, dual-wavelength photometry has been explained, but the invention is not limited to this; a large number of detectors and image-guided optical fibers are provided, and a combination of an appropriate detector and image-guided optical fiber is selected. By using the combination, a wide range of photometry methods can be selected.

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

第1図は固体イメージ検出器を可動とした濃度
計の概略構成図、第2図は本発明の一実施例の概
略構成図である。 2……集光レンズ、3……試料スポツト、4…
…TLCプレート、5……結像レンズ、6……入
口スリツト、6′……スリツト像、7……回折格
子、8……スペクトル像面、9λ1,9λ2……固体
イメージ検出器、10λ1,10λ2……イメージガ
イド形オプチカルフアイバー。
FIG. 1 is a schematic diagram of a densitometer with a movable solid-state image detector, and FIG. 2 is a schematic diagram of an embodiment of the present invention. 2...Condensing lens, 3...Sample spot, 4...
... TLC plate, 5 ... Imaging lens, 6 ... Entrance slit, 6' ... Slit image, 7 ... Diffraction grating, 8 ... Spectral image plane, 9λ 1 , 9λ 2 ... Solid-state image detector, 10λ 1,10λ 2 ...image guide type optical fiber.

Claims (1)

【特許請求の範囲】[Claims] 1 照射された光に基づく試料の像が形成される
入口スリツトと、この入口スリツトを通過した光
を分光する分光素子と、分光された光をそれぞれ
検出する少なくとも一対の上記のスリツト長さ方
向に並べられた固体イメージ検出器とから成る濃
度計において、前記入口スリツトのスペクトル像
に対応する形状の入射端面および出射端面を有す
る少なくとも一対のイメージガイド形オプチカル
フアイバーを設け、各オプチカルフアイバーの入
射端面を前記分光素子によるスペクトル像面上に
おいて波長分散方向に変位自在に配置するととも
に上記各固体イメージ検出器を固定配置し、この
固体イメージ検出器の受光面に前記各イメージガ
イド形オプチカルフアイバーの出射端面をそれぞ
れ対向配置したことを特徴とする濃度計。
1. An entrance slit in which an image of the sample is formed based on the irradiated light, a spectroscopic element that separates the light that has passed through the entrance slit, and at least one pair of the above-mentioned slits that respectively detect the separated lights in the length direction. a densitometer comprising an array of solid-state image detectors, at least a pair of image-guided optical fibers each having an entrance end face and an exit end face each having a shape corresponding to the spectral image of the entrance slit; The above-mentioned solid-state image detectors are arranged so as to be freely displaceable in the wavelength dispersion direction on the spectral image plane of the spectroscopic element, and each of the above-mentioned solid-state image detectors is fixedly arranged, and the output end face of each of the above-mentioned image guide type optical fibers is arranged on the light-receiving surface of the solid-state image detector. A densitometer characterized by being arranged facing each other.
JP17302782A 1982-09-30 1982-09-30 Densitometer Granted JPS5961753A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP17302782A JPS5961753A (en) 1982-09-30 1982-09-30 Densitometer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP17302782A JPS5961753A (en) 1982-09-30 1982-09-30 Densitometer

Publications (2)

Publication Number Publication Date
JPS5961753A JPS5961753A (en) 1984-04-09
JPS6344189B2 true JPS6344189B2 (en) 1988-09-02

Family

ID=15952849

Family Applications (1)

Application Number Title Priority Date Filing Date
JP17302782A Granted JPS5961753A (en) 1982-09-30 1982-09-30 Densitometer

Country Status (1)

Country Link
JP (1) JPS5961753A (en)

Also Published As

Publication number Publication date
JPS5961753A (en) 1984-04-09

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