JPS60213830A - Photodiode array - Google Patents

Photodiode array

Info

Publication number
JPS60213830A
JPS60213830A JP6901484A JP6901484A JPS60213830A JP S60213830 A JPS60213830 A JP S60213830A JP 6901484 A JP6901484 A JP 6901484A JP 6901484 A JP6901484 A JP 6901484A JP S60213830 A JPS60213830 A JP S60213830A
Authority
JP
Japan
Prior art keywords
light
window
receiving surface
photodiode array
stray
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
JP6901484A
Other languages
Japanese (ja)
Inventor
Iwao Kato
加藤 巖
Shigeru Sonobe
園部 茂
Shinji Mayama
真山 新治
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.)
Hitachi Ltd
Original Assignee
Hitachi Ltd
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 Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP6901484A priority Critical patent/JPS60213830A/en
Publication of JPS60213830A publication Critical patent/JPS60213830A/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)
  • Spectrometry And Color Measurement (AREA)
  • Photometry And Measurement Of Optical Pulse Characteristics (AREA)

Abstract

PURPOSE:To make it possible to perform spectrum measurement with high resolution, by forming BPFs in a window, arranging an optical fiber, thereby preventing the inclusion of high-order light, stray light and unnecessary light. CONSTITUTION:A transparent optical fiber 3 having a desired wavelength region is arranged in the vicinity of or in close contact with a window 6 and a light receiving surface 2 of a light receiving element. In the window 6, a stray removing filter 4 and a high-order-light removing filter 5, which have desired transmitting characteristics in correspondence with the desired wavelength region of the light receiving element, are constituted. As a result, the effect of the high-order light, the stray light, which is imparted by the sensitivity difference due to the wavelengths of the photodiode, and the unnecessary light due to the repeating reflections between the light receiving surface 2 and the window 6 can be removed.

Description

【発明の詳細な説明】 〔発明の利用分野〕 分光光度計用の光検出器として用い、測定波長の分散方
向にアレイ状に配列したホトダイオードをシフトレジス
タを用いて純電子的に走査することにより、機構系を用
いないで波長走査させる。
[Detailed Description of the Invention] [Field of Application of the Invention] Used as a photodetector for a spectrophotometer, by purely electronically scanning photodiodes arranged in an array in the dispersion direction of the measurement wavelength using a shift register. , to perform wavelength scanning without using a mechanical system.

〔発明の背景〕[Background of the invention]

ホトダイオードアレイを用いた分光光度計は、機械的な
波長走査が不要で、純電子的に高速波長走査が可能であ
ることから近年分光光度計用として注目されてきた。し
かしながらホトダイオードアレイを分光光度計に使用す
る場合゛、−折格子、プリズム等で分散された光がホト
ダイオードアレイの使用全波長域に常時照射されている
ため次のような問題点が生じてくる。すなわち、(1)
測定波長位置に相当する短波長の高次光の混入。
Spectrophotometers using photodiode arrays have attracted attention in recent years as spectrophotometers because they do not require mechanical wavelength scanning and can perform high-speed wavelength scanning purely electronically. However, when a photodiode array is used in a spectrophotometer, the following problems arise because the entire wavelength range used by the photodiode array is constantly irradiated with light dispersed by folded gratings, prisms, etc. That is, (1)
Contamination with higher-order light with a short wavelength corresponding to the measurement wavelength position.

(2)回折格子等の分散子からの散乱光および分光器内
部の反射光等による迷光が測定波長光への混入。
(2) Stray light due to scattered light from a dispersion element such as a diffraction grating and reflected light inside the spectrometer mixes into the measurement wavelength light.

(3)該窓と受光面とでくり返し反射して測定波長光に
混入してくる不要光。
(3) Unwanted light that is repeatedly reflected by the window and the light-receiving surface and mixed into the measured wavelength light.

等である。etc.

上記問題点を除去するため、(1)一枚の基板上に透過
特性が場所により異なるバンドパスフィルタを受光面に
接して配設する方法、(2)透過帯域が波長によって異
なるガラスフィルタを単色光の分散方向に沿って配列接
合して保護部材を形成し迷光を防止する方法が考えられ
ているが(1)の方法は現実的には受光素子と保護部材
の配線パターン間のワイヤボンデング等のため受光面と
フィルタ面とは相当の間隙が必要であり、一般的に0.
5mm以上の間隙が必要である。迷光、高次光の除去に
は有効であるが該基板と該受光面間のくり返し反射によ
る不要光の除去は困難である。また(2)の方法は、ホ
トダイオードアレイの一素子を単位波長差に対応させよ
うとするとスペクトル像の幅がせまくなり、該ホトダイ
オードアレイの前面にガラスフィルタを置いた場合フィ
ルタの端部における光の屈折1反射によるスペクトル像
の乱れを無視することができなかった。
In order to eliminate the above problems, (1) a method of arranging bandpass filters with transmission characteristics that vary depending on the location on a single substrate in contact with the light-receiving surface; (2) a method of using a monochromatic glass filter with a transmission band that varies depending on the wavelength; A method has been considered to prevent stray light by forming a protective member by arranging and bonding along the direction of light dispersion, but method (1) realistically requires wire bonding between the light receiving element and the wiring pattern of the protective member. etc., a considerable gap is required between the light-receiving surface and the filter surface, which is generally 0.
A gap of 5 mm or more is required. Although it is effective in removing stray light and high-order light, it is difficult to remove unnecessary light due to repeated reflections between the substrate and the light-receiving surface. In addition, in method (2), if one element of the photodiode array is made to correspond to a unit wavelength difference, the width of the spectral image becomes narrow, and if a glass filter is placed in front of the photodiode array, the light at the end of the filter becomes Disturbance of the spectral image due to refraction and reflection could not be ignored.

〔発明の目的〕[Purpose of the invention]

本発明の目的は、ホトダイオードアレイを分光光度計に
使用する場合に生ずる問題点(1)高次光の混入、(2
)回折格子の散乱光および分光内部の反射光による迷光
、(3)窓と受光面間におけるくり返し反射による不要
光の混入。を除去したホトダイオードアレイを提供する
ことである。
The purpose of the present invention is to solve problems that occur when using a photodiode array in a spectrophotometer: (1) mixing of higher order light;
) Stray light due to scattered light from the diffraction grating and reflected light inside the spectrometer; (3) Mixture of unnecessary light due to repeated reflections between the window and the light receiving surface. An object of the present invention is to provide a photodiode array in which the

〔発明の概要〕[Summary of the invention]

本発明はホトダイオードアレイを分光光度計に応用した
場合、純電子的な波長走査が可能なため波長走査のため
の機構系が全く不要というホトダイオードの特徴を生か
すため、単体受光素子使用の分光光度計で行われている
カラーガラスフィルタの切換による迷光、高次光除去の
機構系の採用をやめて、静的な方法により問題点を除去
しアレイホトメータ使用上のメリットを最大限に生かす
方法を考えた。
When the photodiode array is applied to a spectrophotometer, it is possible to perform purely electronic wavelength scanning, and thus a mechanical system for wavelength scanning is completely unnecessary. Instead of adopting a mechanical system for removing stray light and high-order light by switching color glass filters, we devised a static method to eliminate the problems and maximize the benefits of using an array photometer.

〔発明の実施例〕[Embodiments of the invention]

以下、本発明の一実施例を第1図により説明する。図は
ホトダイオードアレイの断面図で受光面の配列方向に切
断した状態を示したものである。
An embodiment of the present invention will be described below with reference to FIG. The figure is a cross-sectional view of a photodiode array cut in the direction in which the light-receiving surfaces are arranged.

図において、lはホト誓イオードアレイで、2は受光面
、3はオプチカルファイバー、4は迷光除去用バンドパ
スフィルタ、5は高次光除去用バンドパスフィルタ、6
は窓、7は保護部材である6ホトダイオードアレイは4
0μmのピッチで512個のホトダイオードが並んだも
のであり、そのうち5’01個のホトダイオードを用い
、該ホトダイオードの範囲に300nn+〜800n+
o&−設定して測定するようになっている。第2図は該
波長範囲における高次光の重なり具合を示す6光源にタ
ングステンランプを使用すると光源の特性から300n
m以下の波長の光は存在しない。従って、ホトダイオー
ドアレイから300nm〜800nw+の波長範囲のス
ペクトルのデータを読み出す場合、高次光に関してはE
i00nm〜800n+nの範囲にあるホトダイオード
に該当する窓面に40On+n以下の波長域で不透明の
バンドパスフィルタ第3図を真空蒸着法により高屈折率
膜として酸化セリウムを、低屈折率膜を弗化マグネシュ
ウムを用い多層膜干渉フィルタを窓に形成し高次光を除
去する。
In the figure, l is a photodiode array, 2 is a light receiving surface, 3 is an optical fiber, 4 is a bandpass filter for removing stray light, 5 is a bandpass filter for removing high-order light, and 6
is the window, 7 is the protective member, 6 photodiode arrays are 4
512 photodiodes are arranged at a pitch of 0 μm, of which 5'01 photodiodes are used, and the range of the photodiodes is 300n+ to 800n+.
It is designed to be measured by setting o&-. Figure 2 shows how high-order light overlaps in the wavelength range. When a tungsten lamp is used as the 6 light sources, the
There is no light with wavelengths less than m. Therefore, when reading spectral data in the wavelength range of 300nm to 800nw+ from a photodiode array, the E
On the window surface corresponding to the photodiode in the range of i00nm to 800n+n, a bandpass filter (Fig. 3) which is opaque in the wavelength range of 40On+n or less is made by vacuum evaporation using cerium oxide as a high refractive index film and magnesium fluoride as a low refractive index film. A multilayer interference filter is formed on the window to remove high-order light.

第4図はホトダイオードの分光感度特性である。FIG. 4 shows the spectral sensitivity characteristics of the photodiode.

短波長域では長波長域に比べて出力差が大きくこのため
、短波長域の測定時、特に400nm以下の波長では長
波長光が散乱し、反射等で測定ダイオードに混入した場
合長波長光の感度が高゛いため僅かの光量でも測定に大
きく影響を与える。このため300ruw〜400nm
波長範囲のホトダイオードに該当する窓面に40On+
n以上の波長域で不透明なバンドパスフィルタ第5図を
前記真空蒸着法で形成させることにより長波長の迷光を
防止する。
The output difference in the short wavelength range is large compared to the long wavelength range. Therefore, when measuring the short wavelength range, especially at wavelengths of 400 nm or less, the long wavelength light will be scattered, and if it enters the measurement diode due to reflection etc., the long wavelength light will be Due to its high sensitivity, even a small amount of light can greatly affect measurements. Therefore, 300ruw~400nm
40On+ on the window surface corresponding to the photodiode in the wavelength range
Stray light of long wavelengths is prevented by forming a bandpass filter (FIG. 5) that is opaque in the wavelength range of n or more by the vacuum evaporation method.

第6図は、ホトダイオードアレイ受光面と窓とのくり返
し反射による不要光の発生を示した概念図である。図で
1はホトダイオードアレイで、2は受光面、6は窓を示
す。L、−L、4は測定光をL4〜LrlはL1〜L3
を測定している時間では不要光となる成分の一部である
。測定波長の受光面2には測定波長光り、〜L3とL4
〜Lrlの測定光より長波長域の不要光も窓と受光面間
でくり返し反射によって同時に入射してくる。不要光の
先妻は測定波長光のそれと比べて極めて小さいが、ホト
ダイオードの分光感度は第4図のように長波長域では短
波長に比べて極めて高い為、不要光による出力は測定波
長340nmで10%以上の大きな値となり測定上大き
な誤差を招く要因となる。
FIG. 6 is a conceptual diagram showing the generation of unnecessary light due to repeated reflections between the photodiode array light receiving surface and the window. In the figure, 1 is a photodiode array, 2 is a light receiving surface, and 6 is a window. L, -L, 4 are measurement lights L4~Lrl are L1~L3
This is part of the component that becomes unnecessary light at the time of measurement. The measurement wavelength light receiving surface 2 has measurement wavelength light, ~L3 and L4.
Unnecessary light in a wavelength range longer than the measurement light of ~Lrl also enters at the same time due to repeated reflections between the window and the light receiving surface. Although the front end of unnecessary light is extremely small compared to that of the measurement wavelength light, the spectral sensitivity of the photodiode is extremely high in the long wavelength range compared to short wavelength as shown in Figure 4, so the output due to unnecessary light is 10 at the measurement wavelength of 340 nm. % or more, which causes a large error in measurement.

第7図はオプチカルファイバーにより上記不要光の混入
を防止した概念図を示す。図において、1はホトダイオ
ードアレイで、2は受光面を、6は窓、3はオプチカル
ファイバー、L、〜L8は測定光を、L4〜しわはり、
−L、を測定している時間では不要光となる成分を示す
。図でオプチカルファイバー3は窓6に接着され、受光
面2に近接して配設されている。受光面とオプチカルフ
ァイバ一端面を近接させることにより、該受光面と該端
面とでくり返し反射による不要光の移動量を押え測定デ
ータに対する誤差の低減を計ることができる。またオプ
チカルファイバー相互間の間隙は光に対して不透明な接
着剤を充填して不要光の回り込みによる妨害を除去する
FIG. 7 shows a conceptual diagram in which mixing of the above-mentioned unnecessary light is prevented by optical fibers. In the figure, 1 is a photodiode array, 2 is a light receiving surface, 6 is a window, 3 is an optical fiber, L, ~L8 is a measurement light, L4 ~ wrinkles,
-L, indicates a component that becomes unnecessary light during the measurement time. In the figure, an optical fiber 3 is bonded to a window 6 and placed close to the light receiving surface 2. By bringing the light-receiving surface and one end surface of the optical fiber close to each other, it is possible to reduce the amount of movement of unnecessary light due to repeated reflections between the light-receiving surface and the end surface, thereby reducing errors in measurement data. In addition, the gaps between the optical fibers are filled with an adhesive that is opaque to light to eliminate interference caused by unnecessary light going around.

上記本実施例によれば、窓に形成されたバンドパスフィ
ルタおよびオプチカルファイバーにより高次光による影
響、ホトダイオードの波長による感度差が与える迷光お
よび受光面と窓との間のくり返し反射による不要光を除
去することにより、高分解能のスペクトル測定が可能な
ホトダイオードアレイを提供するものである。
According to the above embodiment, the bandpass filter and optical fiber formed in the window remove the influence of higher-order light, stray light caused by sensitivity differences depending on the wavelength of the photodiode, and unnecessary light caused by repeated reflections between the light receiving surface and the window. This provides a photodiode array capable of high-resolution spectrum measurement.

〔発明の効果〕〔Effect of the invention〕

本発明によれば、1.高次光が問題となる波長範囲60
0n鵬〜800nmに該当するホトダイオードにバンド
パスフィルタを設は高次光を除去するため、高次光の混
入による測定の誤差が防止できる。2.短波長域300
nm〜400nmに該当するホトダイオードには、長波
長域をカットするバンドパスフィルタを設けであるため
該波長域における迷光による測定誤差を防止できる63
.入射光は窓を透過後オプチカルファイバーによって受
光面まで導かれるため、窓と受光面間でのくり返し反射
による不要光が測定光を混入することを防止できる。
According to the present invention, 1. Wavelength range 60 where higher order light becomes a problem
Since a bandpass filter is provided on the photodiode corresponding to the wavelength range from 0 nm to 800 nm to remove high-order light, measurement errors due to contamination of high-order light can be prevented. 2. Short wavelength range 300
Since the photodiode corresponding to the wavelength range from nm to 400 nm is equipped with a bandpass filter that cuts off the long wavelength range, it is possible to prevent measurement errors due to stray light in the wavelength range63.
.. Since the incident light is guided to the light-receiving surface by the optical fiber after passing through the window, it is possible to prevent unnecessary light from being mixed into the measurement light due to repeated reflections between the window and the light-receiving surface.

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

第1図は本発明になるホトダイオードアレイの横断面図
、第2図は測定波長域に対する2次光の重なり具合を示
す図、第3図は2次光除去フィルタの分光特性図、第4
図はホトダイオードの分光感度特性図、第5図は迷光除
去フィルタの分光特性図、第6図はくり返し反射による
不要光の説明図、第7図はくり返し反射光の除去の説明
図である。 1・・・ホトダイオードアレイ、2・・・受光面、3・
・・オプチカルファイバ、4・・・迷光除去フィルタ、
5・・・高次光除去フィルタ。 代理人 弁理士 高橋明夫 170−
FIG. 1 is a cross-sectional view of the photodiode array according to the present invention, FIG. 2 is a diagram showing how secondary light overlaps with respect to the measurement wavelength range, FIG. 3 is a spectral characteristic diagram of a secondary light removal filter, and FIG.
FIG. 5 is a spectral sensitivity characteristic diagram of a photodiode, FIG. 5 is a spectral characteristic diagram of a stray light removal filter, FIG. 6 is an explanatory diagram of unnecessary light due to repeated reflection, and FIG. 7 is an explanatory diagram of removal of repeatedly reflected light. 1... Photodiode array, 2... Light receiving surface, 3...
...Optical fiber, 4...Stray light removal filter,
5...High-order light removal filter. Agent Patent Attorney Akio Takahashi 170-

Claims (1)

【特許請求の範囲】 1、受光素子と受光素子を保護する部材曾窓で構成され
たホトダイオードアレイにおいて、該窓と受光面に近接
あるいは密着させて所望波長帯域で透明なオプチカルフ
ァイバーを配設し、該窓には素子の所望波長帯域に対応
し所望の透過特性を有するフィルタを構成したことを特
徴とするホトダイオードアレイ。 2、特許請求の範囲第1項に於て、該オプチカルファイ
バーの間瞭に光に不透明な特質を充填したことを特徴と
するホトダイオードアレイ。
[Claims] 1. In a photodiode array consisting of a light-receiving element and a large window that protects the light-receiving element, an optical fiber that is transparent in a desired wavelength band is disposed close to or in close contact with the window and the light-receiving surface. . A photodiode array, characterized in that the window comprises a filter corresponding to a desired wavelength band of the element and having desired transmission characteristics. 2. A photodiode array according to claim 1, characterized in that the optical fiber is filled with a property that is clearly opaque to light.
JP6901484A 1984-04-09 1984-04-09 Photodiode array Pending JPS60213830A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP6901484A JPS60213830A (en) 1984-04-09 1984-04-09 Photodiode array

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP6901484A JPS60213830A (en) 1984-04-09 1984-04-09 Photodiode array

Publications (1)

Publication Number Publication Date
JPS60213830A true JPS60213830A (en) 1985-10-26

Family

ID=13390308

Family Applications (1)

Application Number Title Priority Date Filing Date
JP6901484A Pending JPS60213830A (en) 1984-04-09 1984-04-09 Photodiode array

Country Status (1)

Country Link
JP (1) JPS60213830A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0466403A1 (en) * 1990-07-06 1992-01-15 Optical Coating Laboratory, Inc. Leakage-corrected linear variable filter
DE4223212A1 (en) * 1992-07-15 1994-01-20 Bodenseewerk Perkin Elmer Co Two-beam grating polychromator - has refractive prism for shifting spectrum from diffracting grating, and single octave edge filter in front of two-octave detector array
JP2013124990A (en) * 2011-12-15 2013-06-24 Canon Inc Image processing system and image processing method

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0466403A1 (en) * 1990-07-06 1992-01-15 Optical Coating Laboratory, Inc. Leakage-corrected linear variable filter
DE4223212A1 (en) * 1992-07-15 1994-01-20 Bodenseewerk Perkin Elmer Co Two-beam grating polychromator - has refractive prism for shifting spectrum from diffracting grating, and single octave edge filter in front of two-octave detector array
DE4223212C2 (en) * 1992-07-15 1999-03-18 Bodenseewerk Perkin Elmer Co Grid polychromator
JP2013124990A (en) * 2011-12-15 2013-06-24 Canon Inc Image processing system and image processing method

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