Deprecated: The each() function is deprecated. This message will be suppressed on further calls in /home/zhenxiangba/zhenxiangba.com/public_html/phproxy-improved-master/index.php on line 456
JPH0641916B2 - Spectrofluorometer - Google Patents
[go: Go Back, main page]

JPH0641916B2 - Spectrofluorometer - Google Patents

Spectrofluorometer

Info

Publication number
JPH0641916B2
JPH0641916B2 JP1704684A JP1704684A JPH0641916B2 JP H0641916 B2 JPH0641916 B2 JP H0641916B2 JP 1704684 A JP1704684 A JP 1704684A JP 1704684 A JP1704684 A JP 1704684A JP H0641916 B2 JPH0641916 B2 JP H0641916B2
Authority
JP
Japan
Prior art keywords
wavelength
fluorescence
optical system
side optical
device function
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 - Lifetime
Application number
JP1704684A
Other languages
Japanese (ja)
Other versions
JPS60162942A (en
Inventor
太郎 野上
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 JP1704684A priority Critical patent/JPH0641916B2/en
Publication of JPS60162942A publication Critical patent/JPS60162942A/en
Publication of JPH0641916B2 publication Critical patent/JPH0641916B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime 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
    • G01J3/44Raman spectrometry; Scattering spectrometry ; Fluorescence spectrometry
    • G01J3/4406Fluorescence spectrometry

Landscapes

  • Physics & Mathematics (AREA)
  • Spectroscopy & Molecular Physics (AREA)
  • General Physics & Mathematics (AREA)
  • Investigating, Analyzing Materials By Fluorescence Or Luminescence (AREA)

Description

【発明の詳細な説明】 〔発明の利用分野〕 本発明は分光蛍光光度計に係り、特に測定波長の全域に
わたつて測定スペクトルデータを補正する装置関数を求
めることにより、正確な測定データを求めることが可能
な分光蛍光光度計に関する。
Description: FIELD OF THE INVENTION The present invention relates to a spectrofluorometer, and more particularly, to obtain accurate measurement data by obtaining a device function that corrects measurement spectrum data over the entire measurement wavelength range. Spectrofluorometer capable of

〔発明の背景〕[Background of the Invention]

試料を分析するために励起用光源と、この光源からの励
起光を試料に照射するための励起側分光器からなる励起
側光学系と、この試料から出射される蛍光を分析するた
めに蛍光側分光器、及び蛍光検知器からなる蛍光側光学
系を備えた分光蛍光光度計において、従来行なわれてき
たスペクトル補正方法としては文献「けい光分析」−講
談社サイエンテイフイツク(P81〜87)ーに示され
ているように、まず、光量子計と標準試料(通常の場
合、高濃度のローダミンB)を用いて光源の測定励起光
量を測定することにより励起側光学系の装置関数を求
め、つぎに光量子計を用いて先に求めた測定励起光量に
基づく励起側光学系の装置関数を使用して、蛍光側光学
系の装置関数を(補正関数)を求める光量子計法があ
る。また上記文献に示されているように、蛍光側光学系
の装置関数を求める別な方法として出力既知のタングス
テンランプを用いて、このランプからの光を蛍光側光学
系で測定することにより、この測定値と理論的に求まる
理論値とを比較することにより蛍光側光学系の装置関数
を求めるタングステンランプ方法がある。
An excitation light source for analyzing the sample, an excitation side optical system including an excitation side spectroscope for irradiating the sample with excitation light from this light source, and a fluorescence side for analyzing the fluorescence emitted from this sample In a spectrofluorometer equipped with a fluorescence-side optical system consisting of a spectroscope and a fluorescence detector, a conventional spectrum correction method is described in the literature "Fluorescence analysis" -Kodansha Scientific (P81-87). As shown, first, the device function of the optical system on the excitation side is obtained by measuring the measured excitation light amount of the light source using a photon meter and a standard sample (normally, high concentration Rhodamine B), and then There is an optical quantum meter method in which the device function (correction function) of the fluorescence side optical system is obtained by using the device function of the excitation side optical system based on the measured excitation light amount previously obtained using the optical quantum meter. Further, as shown in the above-mentioned document, using a tungsten lamp whose output is known as another method for obtaining the device function of the fluorescence side optical system, by measuring the light from this lamp with the fluorescence side optical system, There is a tungsten lamp method for obtaining the device function of the fluorescence side optical system by comparing the measured value with a theoretically obtained theoretical value.

しかし、これらの蛍光側光学系の装置関数を求める方法
のうち前者の方法によれば装置関数としては200nm〜
600nmの波長域の関数しか求まらず、後者の方法によ
れば330nm以上の波長域の装置関数しか求められなか
った。
However, according to the former method among the methods for obtaining the device function of these fluorescence side optical systems, the device function is 200 nm to
Only the function in the wavelength region of 600 nm was obtained, and the latter method could only obtain the device function in the wavelength region of 330 nm or more.

このため測定波長全域にわたり蛍光側光学系の装置関数
を求めるためには、2つの方法でそれぞれの装置関数を
求めなければならず、この時、2つの方法の測定結果に
違いがないように、タングステンランプ法に使用する光
源としては、測定する波長域において光量子計法と同じ
測定結果が得られる高性能のタングステンランプを使用
しなければならなかった。
Therefore, in order to obtain the device function of the fluorescence side optical system over the entire measurement wavelength, it is necessary to obtain each device function by two methods. At this time, the measurement results of the two methods should be the same. As a light source used for the tungsten lamp method, a high-performance tungsten lamp that can obtain the same measurement result as that of the photon meter method in the wavelength range to be measured must be used.

〔発明の目的〕[Object of the Invention]

本発明の目的は、分光蛍光光度計の蛍光側光学系の装置
関数を求めるタングステンランプ法の光源として、高性
能のタングステンランプを用いなくても、測定波長の全
域において連続した蛍光側光学系の装置関数を求めて、
測定スペクトルデータ補正を行なうことのできる分光蛍
光光度計を提供することにある。
An object of the present invention is to provide a continuous fluorescence-side optical system in the entire measurement wavelength without using a high-performance tungsten lamp as a light source of a tungsten lamp method for obtaining a device function of a fluorescence-side optical system of a spectrofluorometer. Find the device function,
Another object of the present invention is to provide a spectrofluorometer capable of correcting measured spectrum data.

〔発明の概要〕[Outline of Invention]

本発明の分光蛍光光度計は、試料測定に先立ち光源から
の励起光を標準試料に照射して、光量子計により光源の
励起光量を測定し、つぎにこの光量子計を用いて求めた
光源の励起光量からの励起側光学系の装置関数に基づい
て、短波長から中波長までの蛍光側光学系の装置関数を
求め、また、出力既知の光源からの光を蛍光側光学系で
測定すことより、この測定値と理論値との差から中波長
から長波長までの蛍光側光学系の装置関数を求めること
により、これらの方法が同一対象の光学系装置について
独自に等しく装置関数を求めている中波長領域につい
て、この中波長領域の特定の波長に関して、この特定波
長よりも波長の長い中波長から長波長までの蛍光側光学
系の装置関数と、また、この特定波長よりも波長の短い
短波長から中波長までの蛍光側光学系の装置関数とを用
いて、特定波長におけるこれらの装置関数が合致するよ
うに、これらの装置関数のいずれか一方又は双方を補正
演算して、短波長から長波長まで連続した蛍光側光学系
の装置関数を求めることにより、この装置関数を使用し
て測定スペクトルデータを補正し正確な分析結果を求め
るものである。
The spectrofluorometer of the present invention irradiates a standard sample with excitation light from a light source prior to sample measurement, measures the amount of excitation light of the light source by a photon meter, and then excites the light source obtained using this photon meter. Based on the device function of the excitation side optical system from the amount of light, obtain the device function of the fluorescence side optical system from short wavelength to medium wavelength, also, by measuring the light from the light source of known output with the fluorescence side optical system , By obtaining the device function of the fluorescence side optical system from the middle wavelength to the long wavelength from the difference between the measured value and the theoretical value, these methods uniquely find the same device function for the same target optical system device. Regarding the medium wavelength region, with respect to the specific wavelength in the medium wavelength region, the device function of the fluorescence side optical system with a wavelength longer than the specific wavelength and from the medium wavelength to the long wavelength, and the short wavelength shorter than the specific wavelength. From wavelength to medium wavelength Using the device function of the fluorescence side optical system, so as to match these device functions at a specific wavelength, one or both of these device functions are corrected and calculated, and continuous from a short wavelength to a long wavelength. By obtaining the device function of the fluorescence side optical system, the measured spectrum data is corrected using this device function to obtain an accurate analysis result.

〔発明の実施例〕Example of Invention

本発明の実施例を図面に基づいて説明する。 An embodiment of the present invention will be described with reference to the drawings.

第1図に本発明の実施例の原理図を示す。まず光量子計
と標準試料を用いて励起用光源の測定励起光量を求め、
これに基づく励起側光学系の装置関数を使用して、つぎ
に光量子計法により測定励起光量に基づく励起側光学系
の装置関数から蛍光側光学系の装置関数を求め、さらに
タングステンランプ法によりこの光源の測定値と理論値
との差から装置関数を求めて、これらの2つの装置関数
を500nmで合致させることにより全波長域において連
続した装置関数を求める。
FIG. 1 shows a principle diagram of an embodiment of the present invention. First, using a photon meter and a standard sample, obtain the measured excitation light intensity of the excitation light source,
Using the device function of the excitation-side optical system based on this, then by the photon meter method to obtain the device function of the fluorescence-side optical system from the device function of the excitation-side optical system based on the measured excitation light quantity, further by the tungsten lamp method A device function is obtained from the difference between the measured value of the light source and the theoretical value, and these two device functions are matched at 500 nm to obtain a continuous device function in the entire wavelength range.

これらの装置関数を連続させる方法としては、まず光量
子計法により200nm〜600nmの波長域における装置
の波長特性を測定して、その逆数である蛍光側光学系の
装置関数を記憶装置に記憶させる。つぎにタングステン
ランプ法により500nm以上の波長域における蛍光側光
学系の装置関数を記憶装置に読み込む際に、光量子計法
における500mmの装置関数値とタングステンランプ法
による500mmの装置関数値が一致するようにタングス
テンランプ法の装置関数全体に係数をかけて記憶装置に
記憶させる。このようにして得られた装置関数により2
00mmより800mmまでの測定波長領域の全域において
連続したスペクトル補正が可能となる。
As a method of making these device functions continuous, first, the wavelength characteristic of the device in the wavelength range of 200 nm to 600 nm is measured by the photon measurement method, and the device function of the fluorescence side optical system which is the reciprocal thereof is stored in the storage device. Next, when reading the device function of the fluorescence side optical system in the wavelength range of 500 nm or more by the tungsten lamp method into the storage device, make sure that the device function value of 500 mm in the photonmeter method and the device function value of 500 mm in the tungsten lamp method match. Then, the whole device function of the tungsten lamp method is multiplied by a coefficient and stored in the storage device. The device function thus obtained gives 2
Continuous spectrum correction is possible in the entire measurement wavelength range from 00 mm to 800 mm.

第2図は、本発明に係る分光蛍光光度計の一実施例の構
成を示しており、同図において光源1を出た光は、励起
側分光器2を経て試料室3に導かれ、試料に照射され
る。試料から発する蛍光は、蛍光側分光器6を経て検知
器7に入る。今対象としているのは、蛍光側分光器6と
検知器7よりなる蛍光側光学系の装置関数の補正であ
る。試料室3には、光量子計設置場所4があるが、これ
と別にタングステンランプ設置場所5が存在する。装置
の波長特性データ及び実際の測定データは、ともに検知
器7よりA/D変換器9、バスライン12を経由してR
AM16に読み込まれる。
FIG. 2 shows the configuration of an embodiment of the spectrofluorimeter according to the present invention. In FIG. 2, the light emitted from the light source 1 is guided to the sample chamber 3 via the excitation side spectroscope 2 and the sample Is irradiated. The fluorescence emitted from the sample enters the detector 7 via the fluorescence side spectroscope 6. What is currently targeted is correction of the device function of the fluorescence-side optical system including the fluorescence-side spectroscope 6 and the detector 7. The sample chamber 3 has an optical quantum meter installation place 4, but a tungsten lamp installation place 5 exists separately from this. The wavelength characteristic data of the device and the actual measurement data are both R from the detector 7 via the A / D converter 9 and the bus line 12.
It is read into AM16.

RAM16には励起側光学系の装置関数記憶部17、光
量子計法による蛍光側光学系の装置関数記憶部18、タ
ングステンランプ法による蛍光側光学系の装置関数記憶
部19が独立して設けられている。マイクロプロセツサ
ユニツト(MPU)14はROM15に格納されている
プログラムに基づいてこれら2つの蛍光側光学系の装置
関数のいずれか一方または双方を補正演算して、補正さ
れた装置関数を求めこの装置関数データをRAM16に
記憶させると共にRAM16に記憶された励起側光学系
の装置関数データに基づいて試料の測定データを補正
し、D/A変換器10を介して記憶系11に補正された
スペクトルを記録させる。
The RAM 16 is independently provided with a device function storage unit 17 for the excitation side optical system, a device function storage unit 18 for the fluorescence side optical system by the photon meter method, and a device function storage unit 19 for the fluorescence side optical system by the tungsten lamp method. There is. The microprocessor unit (MPU) 14 corrects and calculates one or both of the device functions of these two fluorescence side optical systems based on a program stored in the ROM 15 to obtain a corrected device function. The function data is stored in the RAM 16, the measurement data of the sample is corrected based on the device function data of the excitation side optical system stored in the RAM 16, and the corrected spectrum is stored in the storage system 11 via the D / A converter 10. Record.

第3図は、上記実施例によれ実際に取つた補正スペクト
ルの例である。広い波長域にあたつた補正スペクトルが
実録されている。このデータは、量子収率算出を目的と
して取られた補正スペクトルであり、スペクトルの裾の
部分まで正しく補正することが必要である。本発明が最
も有効に活用される例の一つである。
FIG. 3 is an example of the correction spectrum actually taken according to the above-mentioned embodiment. The corrected spectrum for a wide wavelength range is actually recorded. This data is a corrected spectrum taken for the purpose of calculating the quantum yield, and it is necessary to correct the bottom of the spectrum correctly. This is one of the examples in which the present invention is most effectively used.

〔発明の効果〕〔The invention's effect〕

本発明の分光蛍光光度計によれば、タングステンランプ
法に使用されるタングステンランプとして長波長から3
30nm付近の短波長まで使用可能な高性能なものを使用
する必要がなく、中波長以上の領域でその出力を出せる
もので十分であり、そして、このタングステンランプか
ら求めた装置関数と、光量子計法で求めた装置関数とが
合致しない場合であっても、測定波長全域において連続
した装置関数が求まる効果がある。
According to the spectrofluorimeter of the present invention, the tungsten lamp used in the tungsten lamp method has a long wavelength range of 3 to 3.
It is not necessary to use a high-performance one that can be used up to a short wavelength of around 30 nm, it is sufficient that it can output its output in the medium wavelength range or more, and the device function obtained from this tungsten lamp and an optical quantum meter Even if the device function obtained by the method does not match, there is an effect that a continuous device function can be obtained in the entire measurement wavelength range.

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

第1図は本発明の原理を説明するための図、第2図は本
発明に係る分光蛍光光度計の一実施例の構成図、第3図
は本発明に係る分光蛍光光度計により得られた補正スペ
クトルの一例を示す図である。 1……光源、2……励起側分光器、3……試料室、6…
…蛍光側分光器、7……検知器、8……機械系制御回
路、9……A/D変換器、10……D/A変換器、14
……MPU、15……ROM、16……RAM。
FIG. 1 is a diagram for explaining the principle of the present invention, FIG. 2 is a configuration diagram of an embodiment of a spectrofluorophotometer according to the present invention, and FIG. 3 is obtained by the spectrofluorophotometer according to the present invention. It is a figure which shows an example of the corrected spectrum. 1 ... Light source, 2 ... Excitation-side spectrometer, 3 ... Sample chamber, 6 ...
... Fluorescence side spectroscope, 7 ... Detector, 8 ... Mechanical system control circuit, 9 ... A / D converter, 10 ... D / A converter, 14
... MPU, 15 ... ROM, 16 ... RAM.

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】励起用光源と、該励起用光源からの励起光
を試料室に設置された試料に照射する励起側分光器を有
する励起側光学系と、前記試料から出射される蛍光を分
析する蛍光側分光器、及び蛍光検知器を有する蛍光側光
学系を備えた分光蛍光光度計において、前記試料室に光
量子計及び出力既知の光源を設け、前記光量子計で得た
前記励起用光源の励起光量に基づいて、励起側光学系の
装置関数を求めて、第一の記憶部に記憶せしめる演算手
段、該演算手段は前記光量子計を用いて前記励起用光源
の励起光量から前記励起側光学系の装置関数に基づき、
短波長から中波長までの前記蛍光側光学系の装置関数を
求めて、第二の記憶部に記憶せしめ、かつ前記出力既知
の光源から照射される光量を前記蛍光側光学系により測
定し、既測定値と理論値との差から中波長から長波長ま
での前記蛍光側光学系の装置関数を求めて、第三の記憶
部に記憶せしめるものであり、前記演算手段は中波長に
おける特定の波長に関して、該特定の波長よりも波長の
長い前記中波長から長波長までの蛍光側光学系の装置関
数と、及び前記特定の波長よりも波長の短い前記短波長
から中波長までの蛍光側光学系の装置関数とを用いて、
前記短波長から中波長までの蛍光側光学系の装置関数
と、前記長波長から中波長までの蛍光側光学系の装置関
数が合致するように、これらの装置関数のいずれか一方
または双方を補正演算して短波長から長波長まで連続し
た蛍光側光学系の装置関数を求めて第四の記憶部に記憶
せしめ、試料測定時に前記第四の記憶部に格納された蛍
光側光学系の装置関数に基づいて測定スペクトルデータ
の補正を行なうことを特徴とする分光蛍光光度計。
1. An excitation-side optical system having an excitation-side light source, an excitation-side spectroscope for irradiating a sample placed in a sample chamber with the excitation light from the excitation-light source, and analyzing fluorescence emitted from the sample. In the spectrofluorometer equipped with a fluorescence-side optical system having a fluorescence-side spectroscope and a fluorescence detector, a photon meter and a light source whose output is known are provided in the sample chamber, and the excitation light source obtained by the photon meter is provided. Based on the pumping light quantity, a device function of the pumping side optical system is obtained, the calculating means for storing in the first storage unit, the calculating means uses the optical quantum meter from the pumping light quantity of the pumping light source to the pumping side optical Based on the system device function,
Obtaining the device function of the fluorescence side optical system from the short wavelength to the medium wavelength, it is stored in the second storage unit, and the amount of light emitted from the light source of the known output is measured by the fluorescence side optical system, From the difference between the measured value and the theoretical value, to obtain the device function of the fluorescence side optical system from the medium wavelength to the long wavelength, is to be stored in the third storage unit, the arithmetic means is a specific wavelength in the intermediate wavelength. With respect to the device function of the fluorescence side optical system from the medium wavelength to the long wavelength having a wavelength longer than the specific wavelength, and the fluorescence side optical system from the short wavelength to the medium wavelength having a wavelength shorter than the specific wavelength. And the device function of
Either or both of these device functions are corrected so that the device function of the fluorescence side optical system from the short wavelength to the medium wavelength and the device function of the fluorescence side optical system from the long wavelength to the medium wavelength match. The device function of the fluorescence-side optical system that was calculated to obtain a continuous fluorescence-side optical system from a short wavelength to a long wavelength is stored in the fourth storage unit, and the device function of the fluorescence-side optical system stored in the fourth storage unit at the time of sample measurement. A spectrofluorometer, which corrects measured spectrum data based on
【請求項2】請求項第1項の分光蛍光光度計において、
前記出力既知の光源として、タングステンランプを用い
たことを特徴とする分光蛍光光度計。
2. The spectrofluorophotometer according to claim 1, wherein
A spectrofluorometer, characterized in that a tungsten lamp is used as the light source whose output is known.
JP1704684A 1984-02-03 1984-02-03 Spectrofluorometer Expired - Lifetime JPH0641916B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1704684A JPH0641916B2 (en) 1984-02-03 1984-02-03 Spectrofluorometer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1704684A JPH0641916B2 (en) 1984-02-03 1984-02-03 Spectrofluorometer

Publications (2)

Publication Number Publication Date
JPS60162942A JPS60162942A (en) 1985-08-24
JPH0641916B2 true JPH0641916B2 (en) 1994-06-01

Family

ID=11933047

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1704684A Expired - Lifetime JPH0641916B2 (en) 1984-02-03 1984-02-03 Spectrofluorometer

Country Status (1)

Country Link
JP (1) JPH0641916B2 (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2012026731A (en) * 2010-07-20 2012-02-09 Hitachi High-Technologies Corp Spectrophotofluorometer and spectrum correction method for the same
JP5772425B2 (en) 2011-09-13 2015-09-02 ソニー株式会社 Fine particle measuring device
JP6015735B2 (en) * 2014-11-07 2016-10-26 ソニー株式会社 Fine particle measuring device

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
田村善蔵外2名編「けい光分析」講談社、昭和49、P81−87

Also Published As

Publication number Publication date
JPS60162942A (en) 1985-08-24

Similar Documents

Publication Publication Date Title
Yappert et al. Correction of polychromatic luminescence signals for inner-filter effects
US2847899A (en) Method of and apparatus for spectrochemical analysis
DE102012007016B3 (en) Optical gas sensor
US3994585A (en) Opto-electrical measuring apparatus for determining the relative hemoglobin content of an illuminated solution by evaluating its light absorption
EP0091126B1 (en) Fluorimeter
JP7056612B2 (en) Turbidity measurement method and turbidity meter
CN114674789B (en) Biological detection method and device based on mobile phone
JPH0641916B2 (en) Spectrofluorometer
Prenna et al. Methodological and instrumentational aspects of cytofluorometry
US5194916A (en) Fluorescence spectrophotometer
JPH0672841B2 (en) Atomic absorption spectrophotometer
JP2003232681A (en) Spectrophotometer
US7289598B2 (en) X-ray fluorescent analysis apparatus
JPS61116627A (en) Fluorescence spectrophotometer
JPH0961351A (en) Moisture content detector, moisture content measurement method and moisture content measurement device
EP0481823A1 (en) Fluorescence measurement apparatus
JPS62278436A (en) Fluorescence light measuring method and apparatus
JP3102485B2 (en) Spectrophotometer
JPH0599627A (en) Measuring apparatus for film thickness
US4178102A (en) Process and apparatus for measuring the concentration of a molecule of selective spectrum in a sample substance
JPH07260680A (en) Infrared sensor
CN113330298A (en) System, method and apparatus for correcting transmission deviation of interference filter due to incident angle
EP0756168A3 (en) Method of measuring amadori compound by light scattering
JPS6280522A (en) spectrofluorometer
SU1173276A1 (en) Method of luminescence spectrum registration and apparatus for accomplishment of same

Legal Events

Date Code Title Description
EXPY Cancellation because of completion of term