JPH0441939B2 - - Google Patents
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- Publication number
- JPH0441939B2 JPH0441939B2 JP11454385A JP11454385A JPH0441939B2 JP H0441939 B2 JPH0441939 B2 JP H0441939B2 JP 11454385 A JP11454385 A JP 11454385A JP 11454385 A JP11454385 A JP 11454385A JP H0441939 B2 JPH0441939 B2 JP H0441939B2
- Authority
- JP
- Japan
- Prior art keywords
- wavelength
- spectrometer
- filter
- waveform
- calibration method
- 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
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- Spectrometry And Color Measurement (AREA)
Description
【発明の詳細な説明】
〔1〕 技術分野
本発明は生体組織の表面に光を当てその反射光
を分光分析することにより生体表層の色素の状態
を分析する装置の改良された波長較正法に係る。[Detailed Description of the Invention] [1] Technical Field The present invention relates to an improved wavelength calibration method for a device that analyzes the state of pigments on the surface of a living body by shining light on the surface of a living tissue and spectroscopically analyzing the reflected light. Related.
〔2〕 従来技術とその問題点
従来本装置の波長較正は干渉フイルタ(ピーク
波長571nm)を用いた波長較正器を使つてその透
過スペクトルのピーク波長に波長軸をあわせる方
法を用いていた。すなわち第2図Aの較正器の干
渉フイルタ21を透過する光のスペクトルは第2
図Bの波形aであつて、そのピーク波長はλ0であ
つて、較正前の波形bを波長δだけずらしaに合
わせることによつて波正較正を行なう。[2] Prior art and its problems Conventionally, the wavelength calibration of this device used a method of aligning the wavelength axis with the peak wavelength of the transmission spectrum using a wavelength calibrator using an interference filter (peak wavelength 571 nm). That is, the spectrum of the light transmitted through the interference filter 21 of the calibrator in FIG.
Waveform a in FIG. B, whose peak wavelength is λ 0 , is subjected to wave calibration by shifting waveform b before calibration by wavelength δ to match a.
然し、上記のλ0とフイルタの厚さtとの間には
λ0=2/3t ……(1)
なる関係があつて、この厚みtはフイルタの製造
ロツトやフイルタの光軸に対する傾きにより均一
とはならず、したがつてピーク波長λ0もバラツキ
があつた。 However, there is a relationship between the above λ 0 and the filter thickness t as follows: λ 0 = 2/3t (1), and this thickness t depends on the manufacturing lot of the filter and the inclination of the filter with respect to the optical axis. It was not uniform, and therefore the peak wavelength λ 0 also varied.
また、このピーク波長λ0にX軸(波長軸)をあ
わせる方法は従来は第3図のように波長ピーク値
(571nm)にカーソルを移動させる操作で行つて
いた。これはかなり感覚的な方法であり、精度が
悪かつた。 Furthermore, the method of aligning the X axis (wavelength axis) with this peak wavelength λ 0 has conventionally been carried out by moving a cursor to the wavelength peak value (571 nm) as shown in FIG. This was a very intuitive method and had poor accuracy.
〔3〕 目的
本考案の目的は分光器の正確かつ再現性の高い
波長較正法を提供することである。[3] Purpose The purpose of the present invention is to provide an accurate and highly reproducible wavelength calibration method for a spectrometer.
〔4〕 問題点を解決するための手段
上記の問題点を解決する本発明の較正方法にお
いては干渉フイルタの厚みに関係なくフイルタを
構成する材料に特有のスペクトル波形を与えるも
のを用いてピーク波長をシフトすることを特徴と
する。このようなフイルタの構成としては例えば
デイデイミウムをガラス基板の表面に蒸着したも
のが特に好適である。その透過スペクトル波形は
第4図のようになる。[4] Means for solving the problems In the calibration method of the present invention that solves the above problems, the peak wavelength is determined by using a filter that gives a spectral waveform specific to the material that makes up the filter, regardless of the thickness of the interference filter. It is characterized by shifting. A particularly suitable structure for such a filter is, for example, one in which deidium is deposited on the surface of a glass substrate. The transmission spectrum waveform is as shown in FIG.
このデイデイミウムフイルタを利用した波長の
自動較正法について以下に述べる第5図で実線の
スペクトル波形はレーザ光線等で較正した分光器
で測定した較正済のスペクトル波形である。この
スペクトルを装置内に記憶しておく。点線のスペ
クトル波形はΔλだけ波長のズレた分光器で測定
した波形である。 The automatic wavelength calibration method using this daymium filter will be described below. In FIG. 5, the solid line spectrum waveform is a calibrated spectrum waveform measured with a spectrometer calibrated with a laser beam or the like. This spectrum is stored in the device. The spectral waveform indicated by the dotted line is a waveform measured with a spectrometer whose wavelength is shifted by Δλ.
ここで較正済のスペクトルの波形をIT(λ)と
し測定した波形をID(λ)として両者の間のシフ
ト量(第5図の斜線を施した部分)IDWを次式で、
使用する透過フイルタの特徴的な透過スペクトル
を有する波長範囲[a,b]について積分するこ
とによつて、算出する。 Here, the calibrated spectrum waveform is IT (λ), the measured waveform is ID (λ), and the shift amount between the two (the shaded area in Figure 5) I DW is calculated using the following formula:
It is calculated by integrating over a wavelength range [a, b] that has a characteristic transmission spectrum of the transmission filter used.
IDW=∫a b〔IT(λ)
−ID(λ+Δλ)〕2dλ ……(2)
今、波長の偏位Δλとシフト量IDWとをプロツト
すると第1図のようになつて
Δλ=0 ……(3)
の時にIDWは最小となる。 I DW =∫ a b [IT (λ) − ID (λ + Δλ)] 2 dλ ...(2) Now, if we plot the wavelength deviation Δλ and the shift amount I DW , we get Δλ= I DW is minimum when 0...(3).
この特性を利用しIDWを計算しこの値を最小に
するようにΔλをシフトしていき、IDWが最小とな
つた時に較正を完了するものとすれば自動的に較
正できる。 Calibration can be performed automatically if I DW is calculated using this characteristic, Δλ is shifted so as to minimize this value, and calibration is completed when I DW becomes minimum.
〔5〕 実施例
前述の原理に基づく実施ステツプのフローチヤ
ートを第6図に示す。[5] Example A flowchart of implementation steps based on the above-mentioned principle is shown in FIG.
以上のステツプで実施した例を第7図に示す。 An example implemented using the above steps is shown in FIG.
〔6〕 効果 高精度の自動的な波長較正が可能となつた。[6] Effect Highly accurate automatic wavelength calibration is now possible.
このことにより高感度で高信頼性の反射スペク
トル測定ができる。また定量的な較正のため再現
性もある。 This allows highly sensitive and reliable reflection spectrum measurement. It is also reproducible due to quantitative calibration.
第1図は波長較正法で計算し較正の判定の基準
とするIDW値と波長のズレΔλとの関係を示す。第
2図Aは従来の波長較正器に用いている干渉フイ
ルタ、同Bは透過スペクトルとその中心波長λ0と
フイルタの厚みtの関係を示す。第3図は従来の
波長較正法の調整のし方について述べたもので、
フイルタのピーク波長に合せてカーソルをシフト
する様子を示す。第4図は本考案の実施例の1つ
として物質固有スペクトルを有すデイデイミウム
フイルタの透過スペクトルを示す。第5図は第4
図のデイデイミウムフイルタを用いた場合の波長
較正法の原理図を示す。第6図は実施ステツプの
フローチヤートを示す。第7図は透過スペクトル
ではなく吸収スペクトルを使用した時の本装置で
の波長較正実施例を示す。
FIG. 1 shows the relationship between the I DW value calculated by the wavelength calibration method and used as a standard for determining calibration and the wavelength deviation Δλ. FIG. 2A shows an interference filter used in a conventional wavelength calibrator, and FIG. 2B shows the transmission spectrum and the relationship between its center wavelength λ 0 and the filter thickness t. Figure 3 describes how to adjust the conventional wavelength calibration method.
This shows how the cursor is shifted according to the peak wavelength of the filter. FIG. 4 shows the transmission spectrum of a deidium filter having a material-specific spectrum as one of the embodiments of the present invention. Figure 5 is the 4th
The principle diagram of the wavelength calibration method when using the deidium filter shown in the figure is shown. FIG. 6 shows a flowchart of the implementation steps. FIG. 7 shows an example of wavelength calibration in this apparatus when using an absorption spectrum instead of a transmission spectrum.
Claims (1)
光器を用いて解析し、組織の状態を診断する組織
分光スペクトル分析装置に用いる波長較正方法に
おいて、較正済の分光器を用いて測定した干渉フ
イルタ透過光のスペクトル波形IT(λ)を計測し
それを記憶する手段と、較正する分光器について
同様にスペクトル波形ID(λ)を計測し、記憶さ
れた前記波形IT(λ)との波長λに関するずれの
積分値IDWを次式により求める手段と、 IDW=∫〔IT(λ)−ID(λ+Δλ)〕2dλ この値が最小になるよう波長をΔλだけ偏位さ
せ波長軸をシフトすることを特徴とする波長較正
方法。 2 波長較正用の干渉フイルタとしてガラス基材
の表面にデイデイミウムを蒸着させたフイルタを
用いることを特徴とする特許請求の範囲第1項記
載の波長較正方法。[Claims] 1. In a wavelength calibration method used in a tissue spectrometer that diagnoses the state of the tissue by projecting light onto living tissue and analyzing the reflected light using a spectrum spectrometer, a calibrated spectrometer is used. The means for measuring and storing the spectral waveform ID (λ) of the light transmitted through the interference filter measured using the calibrated spectrometer, and the means for measuring the spectral waveform ID (λ) of the spectrometer to be calibrated, and the memorized waveform IT (λ) ), and a means for calculating the integral value I DW of the deviation with respect to the wavelength λ from the A wavelength calibration method characterized by shifting the wavelength axis. 2. The wavelength calibration method according to claim 1, characterized in that a filter in which deidiumium is vapor-deposited on the surface of a glass substrate is used as an interference filter for wavelength calibration.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP11454385A JPS61271427A (en) | 1985-05-28 | 1985-05-28 | Wavelength calibration method |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP11454385A JPS61271427A (en) | 1985-05-28 | 1985-05-28 | Wavelength calibration method |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS61271427A JPS61271427A (en) | 1986-12-01 |
| JPH0441939B2 true JPH0441939B2 (en) | 1992-07-09 |
Family
ID=14640403
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP11454385A Granted JPS61271427A (en) | 1985-05-28 | 1985-05-28 | Wavelength calibration method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS61271427A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP6256216B2 (en) * | 2014-06-16 | 2018-01-10 | 株式会社島津製作所 | Spectrometer, liquid chromatograph and spectrometer wavelength calibration method |
-
1985
- 1985-05-28 JP JP11454385A patent/JPS61271427A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS61271427A (en) | 1986-12-01 |
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