JPH01136051A - Immunological reaction measurement using fluctuation of light intensity - Google Patents
Immunological reaction measurement using fluctuation of light intensityInfo
- Publication number
- JPH01136051A JPH01136051A JP29309887A JP29309887A JPH01136051A JP H01136051 A JPH01136051 A JP H01136051A JP 29309887 A JP29309887 A JP 29309887A JP 29309887 A JP29309887 A JP 29309887A JP H01136051 A JPH01136051 A JP H01136051A
- Authority
- JP
- Japan
- Prior art keywords
- light
- sample
- power spectrum
- light intensity
- immune reaction
- 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
Links
- 230000008105 immune reaction Effects 0.000 title claims description 20
- 238000005259 measurement Methods 0.000 title description 10
- 230000003595 spectral effect Effects 0.000 claims abstract description 32
- 238000012545 processing Methods 0.000 claims abstract description 20
- 239000003153 chemical reaction reagent Substances 0.000 claims abstract description 11
- 238000001228 spectrum Methods 0.000 claims abstract description 11
- 238000001514 detection method Methods 0.000 claims abstract description 4
- 239000000126 substance Substances 0.000 claims description 10
- 238000000034 method Methods 0.000 claims description 7
- 238000000691 measurement method Methods 0.000 claims description 4
- 239000010419 fine particle Substances 0.000 claims 1
- 239000012295 chemical reaction liquid Substances 0.000 abstract 1
- 238000009499 grossing Methods 0.000 abstract 1
- 238000011088 calibration curve Methods 0.000 description 5
- 238000010586 diagram Methods 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 230000028993 immune response Effects 0.000 description 2
- 230000003287 optical effect Effects 0.000 description 2
- 238000012935 Averaging Methods 0.000 description 1
- 108010085603 SFLLRNPND Proteins 0.000 description 1
- 239000000427 antigen Substances 0.000 description 1
- 102000036639 antigens Human genes 0.000 description 1
- 108091007433 antigens Proteins 0.000 description 1
- 230000002238 attenuated effect Effects 0.000 description 1
- 238000007796 conventional method Methods 0.000 description 1
- 230000004907 flux Effects 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 239000002245 particle Substances 0.000 description 1
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
この発明は、光強度ゆらぎを用いる免疫反応測定方法に
関する。DETAILED DESCRIPTION OF THE INVENTION [Industrial Field of Application] The present invention relates to a method for measuring an immune reaction using fluctuations in light intensity.
光強度ゆらぎを用いる免疫反応測定方法は、例えば特開
昭6.1−28866号公報において提案され、公知で
ある。この従来の免疫反応測定方法にあっては、サンプ
ルと試薬との反応の前後において反応液中に投射した光
の散乱光強度を検知し、その検知出力をA/D変換した
後高速フーリエ変換(FFT) によりパワースペクト
ル密度を求め、そのパワースペクトル密度の例えば緩和
周波数が反応の前後において抗原抗体反応によって変化
するのを利用して、サンプル中の所定の抗原あるいは抗
体濃度を測定するようにしている。A method for measuring an immune reaction using light intensity fluctuations was proposed in, for example, Japanese Patent Laid-Open No. 6.1-28866, and is well known. In this conventional immune reaction measurement method, the scattered light intensity of light projected into the reaction solution is detected before and after the reaction between the sample and the reagent, and the detected output is A/D converted and then fast Fourier transformed ( The power spectral density is determined by FFT), and the concentration of a given antigen or antibody in a sample is measured by utilizing the fact that, for example, the relaxation frequency of the power spectral density changes due to the antigen-antibody reaction before and after the reaction. .
しかしながら、上述した従来の免疫反応測定方法におい
ては、測定データを多数とらないと、パワースペクトル
密度の統計的なバラツキが大きくなり、高精度の測定が
困難になるという問題がある。また、この問題を解決す
るため、測定データを多数とろうとすると、測定時間が
長くかかると共に、計算処理に要する時間も長くなり、
検体の処理能力が低下するという問題が生じることにな
る。However, in the above-mentioned conventional immune reaction measurement method, there is a problem that unless a large number of measurement data are collected, statistical variations in power spectral density become large, making it difficult to perform highly accurate measurement. In addition, if you try to collect a large amount of measurement data to solve this problem, it will take a long time to measure, and the time required for calculation processing will also increase.
This results in a problem that the sample processing capacity is reduced.
この発明は、このような従来の問題点に着目してなされ
たもので、測定データを多数とることなく、したがって
検体の処理能力を向上させることができると共に、高精
度の測定ができる光強度ゆらぎを用いる免疫反応測定方
法を提供することを目的とする。This invention was made by focusing on these conventional problems, and it is possible to improve the throughput of specimens without collecting a large amount of measurement data, and to improve the light intensity fluctuation that allows highly accurate measurements. The purpose of the present invention is to provide a method for measuring an immune reaction using the method.
〔問題点を解決するための手段及び作用〕上記目的を達
成するため、この発明ではサンプルと試薬とを含む反応
液中に投射した光の散乱光を検出し、その検知出力の強
度ゆらぎのパワースペクトル密度を求めた後、そのパワ
ースペクトル密度をスペクトルウィンドウ処理すること
により統計的な変動の少ない平滑化したパワースペクト
ル密度を得、このパワースペクトル密度に基づいて免疫
反応を測定する。[Means and effects for solving the problem] In order to achieve the above object, the present invention detects the scattered light of the light projected into the reaction solution containing the sample and the reagent, and calculates the power of the intensity fluctuation of the detection output. After determining the spectral density, the power spectral density is subjected to spectral window processing to obtain a smoothed power spectral density with less statistical variation, and the immune response is measured based on this power spectral density.
第1図はこの発明を実施する免疫反応測定装置の一例の
構成を示すものである。この測定装置においては、He
−Neレーザ等の光源1からの光束をハーフミラ−2で
二分し、その一方の光束を信号光としてNOフィルタ3
で減光した後レンズ4によりセル5の中央に集光させ、
他方の光束を参照光としてフォトダイオード6に入射さ
せて光源1の出力光強度のゆらぎをモニタするようにす
る。FIG. 1 shows the configuration of an example of an immune reaction measuring device implementing the present invention. In this measuring device, He
- A light beam from a light source 1 such as a Ne laser is divided into two by a half mirror 2, and one of the beams is used as a signal light by an NO filter 3.
After the light is attenuated by the lens 4, it is focused on the center of the cell 5,
The other luminous flux is made to enter the photodiode 6 as a reference light to monitor fluctuations in the output light intensity of the light source 1.
セル5には、サンプルと、該サンプル中の測定すべき所
定の物質と特異的に結合する物質を含む試薬とを収容し
、このセル5内での微粒子による906敗乱光を、例え
ば直径Q、 3mrnのピンホールを有する一対の円形
スリ7)7a、 7bを経て受光素子8で受光し、セル
5を直接透過する光を光トラップ9で遮断する。なお、
一対の円形スリ7)7a。The cell 5 accommodates a sample and a reagent containing a substance that specifically binds to a predetermined substance to be measured in the sample, and the scattered light 906 caused by the particles in the cell 5 is divided into a diameter Q, for example. The light is received by the light receiving element 8 through a pair of circular slots 7) 7a and 7b having pinholes of 3 mrn, and the light directly transmitted through the cell 5 is blocked by the optical trap 9. In addition,
A pair of circular picks 7) 7a.
7b間の距離はコヒーレンス長とすると共に、これら間
には中空円筒IOを設け、これにより迷光等のノイズを
カセットするようにする。The distance between 7b is set to be the coherence length, and a hollow cylinder IO is provided between these to cassette noise such as stray light.
受光素子8の出力は、低雑音増幅器11で増幅した後、
ローパースフィルタ12を通して高周波雑音をカットし
、次に再び増幅器13で増幅した後、A/D変換器14
でデジタル信号に変換してコンピュータ15に供給する
。コンピュータ15では、A/D変換器14からのデジ
タル信号を基にFFTを行ってパワースペクトル密度を
求めると共に、得られたパワースペクトル密度を何回か
平均して統計的な変動を抑えた後、そのパワースペクト
ル密度をスペクトルウィンドウ処理し、次にこのスペク
トルウィンドウ処理によって求めたパワースペクトル密
度を、S/Nを向上させるために平滑化処理する。After the output of the light receiving element 8 is amplified by the low noise amplifier 11,
After cutting high frequency noise through a low-pass filter 12 and then amplifying it again with an amplifier 13, the A/D converter 14
The signal is converted into a digital signal and supplied to the computer 15. The computer 15 performs FFT on the digital signal from the A/D converter 14 to obtain the power spectrum density, and after averaging the obtained power spectrum density several times to suppress statistical fluctuations, The power spectral density is subjected to spectral window processing, and then the power spectral density obtained by this spectral window processing is smoothed in order to improve the S/N.
この実施例では、スペクトルウィンドウ処理としてハニ
ングウィンドウ処理を行う。すなわち、FFTにより求
めたパワースペクトル密度の値を、周波数の低い方から
順番にAt、 A2. A3. 。In this embodiment, Hanning window processing is performed as the spectral window processing. That is, the values of the power spectral densities obtained by FFT are divided into At, A2. A3. .
、 ANとすると、これらのデータを用いてハニング
ウィンドウ処理を行って、
B1=0.5八t+o、5A2
B2=0.25A1+0.5A2+0.25A3B3=
0.25A2+0.5A3+0.25A48N=0.5
A (N−1) +Q、 5ANを求め、このパワース
ペクトル密度Bl、 B2. B3゜、ONに基づいて
免疫反応を測定する。, AN, perform Hanning window processing using these data, B1=0.58t+o, 5A2 B2=0.25A1+0.5A2+0.25A3B3=
0.25A2+0.5A3+0.25A48N=0.5
A (N-1) +Q, 5AN is determined, and this power spectrum density Bl, B2. Measure the immune response based on B3°, ON.
第2図Aはハニングウィンドウ処理を行ったパワースペ
クトル密度を、第2図Bはハニングウィンドウ処理を行
う前、すなわち従来の測定方法によるパワースペクトル
密度を示すもので、それぞれCRP抗原濃度が4 Xl
0−6g/mlのサンプルと試薬との反応開始前(破線
)と反応後15分(実線)の測定データを示すものであ
る。第2図A、Bから明らかなように、ハウニングウィ
ンドウ処理を行えば、限られた測定データから統計的な
変動の小さい平滑化されたパワースペクトル密度を得る
ことできるので、そのパワースペクトル密度に基づいて
免疫反応の有無およびその濃度を高精度で測定すること
ができる。Figure 2A shows the power spectral density after Hanning window processing, and Figure 2B shows the power spectral density before Hanning window processing, that is, according to the conventional measurement method.
It shows measurement data before the start of the reaction between a 0-6 g/ml sample and a reagent (dashed line) and 15 minutes after the reaction (solid line). As is clear from Figures 2A and B, by performing the houning window process, it is possible to obtain a smoothed power spectral density with small statistical fluctuations from limited measurement data. Based on this, the presence or absence of an immune reaction and its concentration can be measured with high accuracy.
ここで、免疫反応p有無およびその所定の物質の濃度は
、例えば以下のようにして測定することができる。Here, the presence or absence of an immune reaction and the concentration of a predetermined substance can be measured, for example, as follows.
1)サンプルと試薬との反応後における緩和周波数(低
周波数領域における平坦なレベル(ホワイトレベル)か
ら3dB低下したパワースペクトル密度を示す周波数)
を求め、予め求めた濃度と緩和周波数との検量線から免
疫反応の有無およびサンプル中の所定の物質の濃度を決
定する。1) Relaxation frequency after the reaction between sample and reagent (frequency that indicates a power spectral density that is 3 dB lower than a flat level (white level) in the low frequency region)
The presence or absence of an immune reaction and the concentration of a predetermined substance in the sample are determined from a calibration curve of the concentration determined in advance and the relaxation frequency.
li)サンプルと試薬との反応後におけるホワイトレベ
ルの平均値あるいは積分値を求め、予め求めた濃度とホ
ワイトレベルの平均値あるいは積分値との検量線から免
疫反応の有無およびサンプル中の所定の物質の濃度を決
定する。li) Calculate the average value or integral value of the white level after the reaction between the sample and the reagent, and determine the presence or absence of an immune reaction and the specified substance in the sample from a calibration curve between the concentration determined in advance and the average value or integral value of the white level. Determine the concentration of
iii )サンプルと試薬との反応前後における緩和周
波数の比を求め、予め求めた濃度と緩和周波数比との検
量線から免疫反応の有無およびサンプル中の所定の物質
の濃度を決定する。iii) The ratio of relaxation frequencies before and after the reaction between the sample and the reagent is determined, and the presence or absence of an immune reaction and the concentration of a predetermined substance in the sample are determined from a calibration curve of the concentration determined in advance and the relaxation frequency ratio.
iv)サンプルと試薬との反応前後におけるホワイトレ
ベルの平均値あるいは積分値の比を求め、予め求めた濃
度とホワイトレベルの平均値あるいは積分値比との検量
線から免疫反応の有無およびサンプル中の所定の物質の
濃度を決定する。iv) Calculate the ratio of the average value or integral value of the white level before and after the reaction between the sample and the reagent, and use the calibration curve between the predetermined concentration and the average value or integral value ratio of the white level to determine the presence or absence of an immune reaction and the concentration of the white level in the sample. Determine the concentration of a given substance.
■)サンプルと試薬との反応前後における相対ゆらぎの
比を求め、予め求めた濃度と相対ゆらぎ比との検量線か
ら免疫反応の有無およびサンプル中の所定の物質の濃度
を決定する。(2) The ratio of relative fluctuation before and after the reaction between the sample and the reagent is determined, and the presence or absence of an immune reaction and the concentration of a predetermined substance in the sample are determined from a calibration curve of the concentration determined in advance and the relative fluctuation ratio.
なお、この発明は上述した実施例にのみ限定されるもの
ではな(、幾多の変更または変形が可能である。例えば
、上述した実施例ではスペクトルウィンドウ処理として
ハミングウィンドウ処理を行うようにしたが、ハミング
ウィンドウ処理を行うこともできる。この場合には、F
FTにより求めたパワースペクトル密度Al、 A2.
A3. − 、AN ニ基づいて、
叫=0.54A1+0.54八2
C2=0.23A1+0.54A2+0.23A3C3
=0.23A2+0.54A3+0.23八4CN=0
.54A (N−1) +0.54ANのパワースペク
トル密度を求めればよい。また、その他のスペクトルウ
ィンドウとして、例えば箱型ウィンドウや赤池のウィン
ドウ等を適用することもできる。Note that the present invention is not limited to the above-mentioned embodiments (many changes and modifications are possible). For example, in the above-mentioned embodiments, Hamming window processing is performed as the spectral window processing. Hamming window processing can also be performed.In this case, F
Power spectrum density Al obtained by FT, A2.
A3. - Based on AN 2, C2 = 0.54A1 + 0.5482 C2 = 0.23A1 + 0.54A2 + 0.23A3C3
=0.23A2+0.54A3+0.2384CN=0
.. The power spectral density of 54A (N-1) +0.54AN may be found. Further, as other spectrum windows, for example, a box-shaped window, an Akaike window, etc. can also be applied.
以上述べたように、この発明によれば検知出力の強度ゆ
らぎのパワースペクトル密度をスペクトルウィンドウ処
理するようにしたので、限られた測定データから統計的
なバラツキの少ない平滑化されたパワースペクトル密度
を簡単に得ることができる。したがって、測定データを
多くすることなく、免疫反応を高精度で測定することが
できると共に、検体の処理能力も向上できる。As described above, according to the present invention, the power spectral density of the intensity fluctuation of the detection output is subjected to spectral window processing, so that a smoothed power spectral density with less statistical variation can be obtained from limited measurement data. can be obtained easily. Therefore, the immune reaction can be measured with high accuracy without increasing the amount of measurement data, and the processing capacity of the specimen can also be improved.
第1図はこの発明を実施する免疫反応測定装置の一例の
構成を示すブロック図、
第2図AおよびBはこの発明によるパワースペクトル密
度と従来法によるパワースペクトル密度とを比較して示
す図である。
■・・・光源 2・・・ハーフミラ−3・
・・N、Dフィルタ 4・・・レンズ5・・・セル
6・・・フォトダイオード7a、 7b
・・・円形スリット 訃・・受光素子9・・・光トラッ
プ 10・・・中空円筒11・・・低雑音増幅器
12・・・ローパスフィルタ13・・・増幅器
14・・・A/D変換器15・・・コンピュ
ータ
第1図
第2図
周yL牧(Hz)Fig. 1 is a block diagram showing the configuration of an example of an immune reaction measuring device implementing the present invention, and Figs. 2 A and B are diagrams showing a comparison of the power spectral density according to the present invention and the power spectral density according to the conventional method. be. ■...Light source 2...Half mirror 3.
...N, D filter 4...Lens 5...Cell 6...Photodiode 7a, 7b
... Circular slit ... Photodetector 9 ... Optical trap 10 ... Hollow cylinder 11 ... Low noise amplifier 12 ... Low pass filter 13 ... Amplifier
14... A/D converter 15... Computer Figure 1 Figure 2 Frequency (Hz)
Claims (1)
結合する物質を含む試薬との反応液中に光を投射して、
該反応液中に存在する微粒子による散乱光を検出し、そ
の検知出力の強度ゆらぎのパワースペクトル密度を求め
た後、そのパワースペクトル密度をスペクトルウィンド
ウ処理し、このスペクトルウィンドウ処理して得たパワ
ースペクトル密度に基づいて免疫反応を測定することを
特徴とする光強度ゆらぎを用いる免疫反応測定方法。 2、前記スペクトルウィンドウをハニングウィンドウと
することを特徴とする特許請求の範囲第1項記載の光強
度ゆらぎを用いる免疫反応測定方法。 3、前記スペクトルウィンドウをハミングウィンドウと
することを特徴とする特許請求の範囲第1項記載の光強
度ゆらぎを用いる免疫反応測定方法。[Claims] 1. Projecting light into a reaction solution of a sample and a reagent containing a substance that specifically binds to a predetermined substance in the sample,
After detecting the light scattered by the fine particles present in the reaction solution and determining the power spectral density of the intensity fluctuation of the detection output, the power spectral density is subjected to spectral window processing, and the power spectrum obtained by this spectral window processing is An immune reaction measurement method using light intensity fluctuation, characterized in that the immune reaction is measured based on density. 2. The immune reaction measuring method using light intensity fluctuation according to claim 1, wherein the spectral window is a Hanning window. 3. The immune reaction measuring method using light intensity fluctuation according to claim 1, wherein the spectral window is a Hamming window.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP29309887A JPH01136051A (en) | 1987-11-21 | 1987-11-21 | Immunological reaction measurement using fluctuation of light intensity |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP29309887A JPH01136051A (en) | 1987-11-21 | 1987-11-21 | Immunological reaction measurement using fluctuation of light intensity |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH01136051A true JPH01136051A (en) | 1989-05-29 |
Family
ID=17790397
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP29309887A Pending JPH01136051A (en) | 1987-11-21 | 1987-11-21 | Immunological reaction measurement using fluctuation of light intensity |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH01136051A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2010092950A1 (en) * | 2009-02-13 | 2010-08-19 | 興和株式会社 | Method for assaying physiological substance of biological origin and assay device therefor |
-
1987
- 1987-11-21 JP JP29309887A patent/JPH01136051A/en active Pending
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2010092950A1 (en) * | 2009-02-13 | 2010-08-19 | 興和株式会社 | Method for assaying physiological substance of biological origin and assay device therefor |
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