JPH04301744A - Prism for micro-total refection measurement - Google Patents

Prism for micro-total refection measurement

Info

Publication number
JPH04301744A
JPH04301744A JP3091294A JP9129491A JPH04301744A JP H04301744 A JPH04301744 A JP H04301744A JP 3091294 A JP3091294 A JP 3091294A JP 9129491 A JP9129491 A JP 9129491A JP H04301744 A JPH04301744 A JP H04301744A
Authority
JP
Japan
Prior art keywords
reflecting surface
light
incident
measurement
sample
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.)
Granted
Application number
JP3091294A
Other languages
Japanese (ja)
Other versions
JP3039569B2 (en
Inventor
Koji Suzuki
康志 鈴木
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 JP9129491A priority Critical patent/JP3039569B2/en
Publication of JPH04301744A publication Critical patent/JPH04301744A/en
Application granted granted Critical
Publication of JP3039569B2 publication Critical patent/JP3039569B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Abstract

PURPOSE:To enable micro total-reflection measurement with the two kinds, large and small, of incident angles by the use of the same prism without attenuation. CONSTITUTION:A device is provided with a first reflecting surface 3 by which incident light is totally reflected, a second reflecting surface 4 which faced to the first reflecting surface 3 while incident light is totally reflected, and with a third reflecting surface 5 which is faced to the second reflecting surface 4 while light is totally reflected to a light emission surface, and the device is so designed that specimens can be adhered and fixed onto the second reflecting surface 4 and the first reflecting surface 3. Since incident light comes in the first and the third reflecting surfaces 3 and 5 at a comparatively large incident angle, and since light comes in the second reflecting surface 4 at a comparatively small incident angle, if the specimens are adhered and fixed onto the first and the third reflecting surfaces 3 and 5, measurement by the comparatively large incident angle can thereby be made, and if the specimen is adhered and fixed onto the second reflecting surface 4, measurement by the comparatively small incident angle can thereby be made. Furthermore, when a position from which light is radiated to the plane of incidence 2, is changed, a part of light does not come in the third reflecting surface 5 while no light comes in a detector, measurement can thereby be made while the range of the specimen is being selected.

Description

【発明の詳細な説明】[Detailed description of the invention]

【0001】0001

【産業上の利用分野】本発明は、試料の微小領域に光を
照射して定性分析を行なう顕微方式に適した全反射測定
用のプリズムに関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a prism for measuring total reflection, which is suitable for a microscopic method in which qualitative analysis is performed by irradiating light onto a minute area of a sample.

【0002】0002

【従来の技術】微小な試料に対する全反射測定において
は、試料を密着させたプリズムに光源からの光をビーム
コンデンサにより絞り込んで入射させ、試料により吸光
を受けた光を検出することが行なわれているが、プリズ
ムに入射した光ビームは、プリズム中で拡散するため、
試料全体についての測定結果となってしまって試料の微
小領域を特定した分析ができないという問題がある。こ
のような問題を解消するために断面「く」の字状に形成
されたプリズムを用い、これに試料を密着させて測定す
るようにしている。これによれば、赤外線を照射する箇
所を選択することができる反面、出射までに4回もの全
反射回数を必要とするために必然的に光路長が大きくな
って減衰を招くという問題のほかに、炭素を含んだよう
な屈折率の高い試料への適用が困難であった。
[Prior Art] In total reflection measurement for a minute sample, light from a light source is focused by a beam condenser and incident on a prism with the sample in close contact with it, and the light absorbed by the sample is detected. However, since the light beam incident on the prism is diffused within the prism,
There is a problem in that the measurement results are for the entire sample, making it impossible to analyze a specific micro region of the sample. To solve this problem, a prism with a dogleg-shaped cross section is used, and the sample is brought into close contact with the prism for measurement. According to this, while it is possible to select the location where infrared rays are irradiated, there is the problem that the optical path length inevitably increases because it requires four total reflections before it is emitted, causing attenuation. However, it was difficult to apply this method to samples with a high refractive index, such as those containing carbon.

【0003】0003

【発明が解決しようとする課題】本発明はこのような事
情に鑑みてなされたものであって、その目的とするとこ
ろは試料の測定領域の特定が可能で、しかも入射から出
射までの光路長を小さくして減衰を小さくでき、さらに
同一のプリズムにより大小複数種類の入射角による測定
を可能ならしめる新規な顕微全反射測定用プリズムを提
供することである。
[Problems to be Solved by the Invention] The present invention has been made in view of the above circumstances, and its purpose is to make it possible to specify the measurement area of a sample, and to reduce the optical path length from input to output. It is an object of the present invention to provide a new prism for microscopic total internal reflection measurement, which can reduce attenuation by reducing the angle of incidence, and further enables measurement with a plurality of large and small types of incident angles using the same prism.

【0004】0004

【課題を解決するための手段】このような問題を解消す
るために本発明においては、入射光に対して全反射を行
なう第1の反射面と、第1の反射面に対向するとともに
全反射を行なう第2の反射面と、第2の反射面に対向す
るとともに出射面に全反射を行なう第3の反射面とを備
え、少なくとも第2、及び第1、または第3の反射面に
試料を密着、固定可能に構成するようにした。
[Means for Solving the Problems] In order to solve such problems, the present invention includes a first reflective surface that totally reflects incident light, and a surface that faces the first reflective surface and that completely reflects the incident light. a second reflecting surface that performs total reflection, and a third reflecting surface that faces the second reflecting surface and performs total reflection on the output surface, and a sample is placed on at least the second, first, or third reflecting surface. The structure is designed to allow for close contact and fixation.

【0005】[0005]

【作用】第1、第3の反射面は入射光に対して比較的大
きな入射角で光が入射し、また第2の反射面は比較的小
さな入射角で光が入射するから、第1、第3の反射面に
試料を密着、固定すると、比較的大きな入射角による測
定が、また第1の反射面に試料を密着、固定すると、比
較的小さな入射角による測定が可能となる。また、光源
からの光を入射させる位置を変えることにより、光の一
部が第3の反射面に到達しなくなって検出器に入射しな
くなるから、試料の領域を選択しながら測定することが
可能となる。
[Operation] Since light enters the first and third reflecting surfaces at a relatively large angle of incidence relative to the incident light, and light enters the second reflecting surface at a relatively small angle of incidence, the first and third reflecting surfaces When the sample is closely attached and fixed to the third reflecting surface, measurement can be performed at a relatively large angle of incidence, and when the sample is closely attached and fixed to the first reflecting surface, measurement can be carried out at a relatively small angle of incidence. In addition, by changing the incident position of the light from the light source, some of the light no longer reaches the third reflective surface and enters the detector, making it possible to select and measure areas of the sample. becomes.

【0006】[0006]

【実施例】そこで以下に本発明の詳細を図示した実施例
に基づいて説明する。図1は、本発明の一実施例を示す
ものであって、図中符号1は赤外線が透過可能な光学材
料、例えばKRS−5や、ZnSe、ZnSにより断面
「M」字状に形成された赤外顕微全反射測定用プリズム
であって、入射面2にから入射した赤外線に対して全反
射を生じる角度で第1の反射面3が形成されている。こ
の反射面3は、入射面2に対して30度の角度となるよ
うに反射面が設定され、これにより赤外光が60度の角
度で入射することになる。第1の反射面3と対向する側
には入射面2に対しては直角で、かつ第1の反射面3か
らの赤外線を全反射する角度、例えば入射角45度とな
るように第2の反射面4が形成され、更に第1の反射面
3に隣接する側には第2の反射面4により反射された赤
外光を出射面6に対して全反射する角度、例えば60度
の入射角となるように第3の反射面5が形成されている
DESCRIPTION OF THE PREFERRED EMBODIMENTS The details of the present invention will be explained below based on illustrated embodiments. FIG. 1 shows an embodiment of the present invention, in which reference numeral 1 is made of an optical material that can transmit infrared rays, such as KRS-5, ZnSe, or ZnS, and has an "M"-shaped cross section. This is a prism for infrared microscopic total reflection measurement, and a first reflecting surface 3 is formed at an angle that causes total reflection of infrared rays incident from an incident surface 2. The reflective surface 3 is set to form an angle of 30 degrees with respect to the incident surface 2, so that the infrared light is incident at an angle of 60 degrees. On the side facing the first reflective surface 3, there is a second surface at a right angle to the incident surface 2 and at an angle that totally reflects the infrared rays from the first reflective surface 3, for example, at an incident angle of 45 degrees. A reflective surface 4 is formed, and further, on the side adjacent to the first reflective surface 3, there is an incident angle, for example, 60 degrees, for total reflection of the infrared light reflected by the second reflective surface 4 toward the output surface 6. A third reflective surface 5 is formed to form a corner.

【0007】この実施例において、比較的小さな入射角
を必要とする試料を測定する場合には、図2の(イ)に
示したように試料S1を第1の反射面2に密着させて固
定する。この状態で入射面2から入射した赤外光は、第
1の反射面3で反射されて第2の反射面4に約45度の
比較的小さな入射角でもって入射する。これにより第2
の反射面4に密着固定されている試料S1に比較的小さ
な入射角で赤外線が入射し、試料の特性に対応した波長
の成分が吸収され、他の波長成分が反射されて第3の反
射面5に反射されて出射面6から外部に出る。これによ
り比較的小さな入射角で赤外線の入射を必要とする試料
の全反射測定が行なわれることになる。
In this embodiment, when measuring a sample that requires a relatively small angle of incidence, the sample S1 is fixed in close contact with the first reflective surface 2 as shown in FIG. do. In this state, the infrared light that enters from the incident surface 2 is reflected by the first reflective surface 3 and enters the second reflective surface 4 at a relatively small incident angle of about 45 degrees. This allows the second
Infrared rays are incident at a relatively small incident angle on the sample S1, which is closely fixed to the reflective surface 4 of 5 and exits from the exit surface 6. As a result, total reflection measurement of the sample, which requires the incidence of infrared rays at a relatively small angle of incidence, can be performed.

【0008】一方、大きな入射角での測定が必要な場合
には、図2の(ロ)に示したように第1の反射面3に試
料Sを密着、固定すると、反射面3が入射光に対して比
較的大きな入射角を有しているから、試料S2に60度
という大きな入射角で入射することになる。試料の特性
に応じて波長成分の一部が吸収され、残りの成分は第2
の反射面4、第3の反射面5で反射されて出射面から外
部に出射することになる。なお、同図(ハ)に示したよ
うに複数の反射面3、5に試料を密着、固定することに
より、試料に多重回の吸収を行なわせて高い感度での測
定が可能となる。
On the other hand, when measurement at a large angle of incidence is required, the sample S is tightly attached and fixed to the first reflective surface 3 as shown in (b) of FIG. Since it has a relatively large incident angle with respect to the sample S2, it will be incident on the sample S2 at a large incident angle of 60 degrees. Depending on the characteristics of the sample, some of the wavelength components are absorbed, and the remaining components are absorbed by the second wavelength component.
The light is reflected by the reflective surface 4 and the third reflective surface 5, and is emitted to the outside from the output surface. By the way, as shown in FIG. 3C, by closely contacting and fixing the sample to a plurality of reflective surfaces 3 and 5, the sample can absorb multiple times, making it possible to perform measurements with high sensitivity.

【0009】ところで、反射面に取り付けられた試料の
一部について測定したい場合には、図3に示したように
光源からの光ビームを入射させる入射面2上の位置をず
らせることにより、第2の反射面4で反射された赤外線
の一部が第3の反射面5に到達しなくなって検出器に入
射しなくなる。これにより、試料の領域を特定した測定
が可能となる。
By the way, when it is desired to measure a part of the sample attached to the reflective surface, as shown in FIG. A part of the infrared rays reflected by the second reflecting surface 4 no longer reaches the third reflecting surface 5 and is no longer incident on the detector. This makes it possible to measure a specific region of the sample.

【0010】なお、この実施例においては赤外線による
測定に例を採って説明したが、可視光透過性材料により
構成することにより、可視光線による分析にも適用でき
ることは明かである。
Although this embodiment has been explained by taking an example of measurement using infrared rays, it is obvious that it can also be applied to analysis using visible light by constructing it from a material that transmits visible light.

【0011】[0011]

【発明の効果】以上説明したように本発明においては、
入射光に対して全反射を行なう第1の反射面と、第1の
反射面に対向するとともに全反射を行なう第2の反射面
と、第2の反射面に対向するとともに出射面に全反射を
行なう第3の反射面とを備え、少なくとも第2、及び第
1、または第3の反射面に試料を密着、固定可能に構成
したので、第1、もしくは第3の反射面は入射光に対し
て比較的大きな入射角で光が入射し、また第2の反射面
は比較的小さな入射角で光が入射するから、第1、第3
の反射面に試料を密着、固定すると、比較的大きな入射
角による測定が、また第2の反射面に試料を密着、固定
すると、比較的小さな入射角による測定が可能となり、
試料を取り付ける面を変えるだけで試料への入射角を変
更することができる。また、光源からの光を入射させる
位置を変えることにより、光の一部が第3の反射面に到
達しなくなって検出器に入射しなくなるから、試料の領
域を選択しながら測定することができる。
[Effects of the Invention] As explained above, in the present invention,
A first reflective surface that totally reflects the incident light; a second reflective surface that faces the first reflective surface and that totally reflects the incident light; and a second reflective surface that faces the second reflective surface and totally reflects the incident light. Since the sample is configured to be able to be closely attached and fixed to at least the second, first, or third reflecting surface, the first or third reflecting surface is not exposed to the incident light. On the other hand, light is incident on the second reflecting surface at a relatively large incident angle, and light is incident on the second reflecting surface at a relatively small incident angle.
When the sample is closely attached and fixed to the second reflecting surface, measurements can be made at a relatively large angle of incidence, and when the sample is attached and fixed to the second reflecting surface, measurements can be made at a relatively small angle of incidence.
The angle of incidence on the sample can be changed simply by changing the surface on which the sample is mounted. Additionally, by changing the incident position of the light from the light source, a portion of the light no longer reaches the third reflective surface and enters the detector, making it possible to select and measure areas of the sample. .

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

【図1】本発明の一実施例を示す側面図である。FIG. 1 is a side view showing one embodiment of the present invention.

【図2】同図(イ)、(ロ)、及び(ハ)は、それぞれ
同上プリズムの使用状態を示す説明図である。
FIG. 2A, FIG. 2B, and FIG. 2C are explanatory diagrams each showing how the prism is used.

【図3】試料の特定領域を選択して測定する場合の動作
を示す説明図である。
FIG. 3 is an explanatory diagram showing the operation when selecting and measuring a specific region of a sample.

【符号の説明】[Explanation of symbols]

1  プリズム本体 2  入射面 3  第1の反射面 4  第2の反射面 5  第3の反射面 6  出射面 S1 、S2  試料 1 Prism body 2 Incidence surface 3 First reflective surface 4 Second reflective surface 5 Third reflective surface 6 Output surface S1, S2 samples

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】  入射光に対して全反射を行なう第1の
反射面と、第1の反射面に対向するとともに全反射を行
なう第2の反射面と、第2の反射面に対向するとともに
出射面に全反射を行なう第3の反射面とを備え、少なく
とも第2、及び第1、または第3の反射面に試料を密着
、固定可能に構成してなる顕微全反射測定用プリズム。
Claim 1: a first reflective surface that totally reflects incident light; a second reflective surface that faces the first reflective surface and that performs total internal reflection; and a second reflective surface that faces the second reflective surface and that 1. A prism for microscopic total internal reflection measurement, comprising a third reflecting surface that performs total reflection on an output surface, and configured such that a sample can be brought into close contact with and fixed to at least the second, first, or third reflecting surface.
JP9129491A 1991-03-29 1991-03-29 Prism for total internal reflection measurement Expired - Lifetime JP3039569B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9129491A JP3039569B2 (en) 1991-03-29 1991-03-29 Prism for total internal reflection measurement

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9129491A JP3039569B2 (en) 1991-03-29 1991-03-29 Prism for total internal reflection measurement

Publications (2)

Publication Number Publication Date
JPH04301744A true JPH04301744A (en) 1992-10-26
JP3039569B2 JP3039569B2 (en) 2000-05-08

Family

ID=14022454

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9129491A Expired - Lifetime JP3039569B2 (en) 1991-03-29 1991-03-29 Prism for total internal reflection measurement

Country Status (1)

Country Link
JP (1) JP3039569B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2008224451A (en) * 2007-03-13 2008-09-25 Hamamatsu Photonics Kk Device for measuring terahertz wave

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
TWM505240U (en) * 2014-09-10 2015-07-21 Zhi-Xiong Yu Combinational cabinet connector

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2008224451A (en) * 2007-03-13 2008-09-25 Hamamatsu Photonics Kk Device for measuring terahertz wave

Also Published As

Publication number Publication date
JP3039569B2 (en) 2000-05-08

Similar Documents

Publication Publication Date Title
CA1321488C (en) Biological sensors
US3604927A (en) Total reflection fluorescence spectroscopy
US6819422B2 (en) Measuring method for immunochromatographic test strip
JP3474880B2 (en) Optical device for performing immunoassays
JPH1096695A (en) Method for measuring scattering light
KR960705200A (en) Surface thermal inspection device
US5039225A (en) Apparatus for measurement of reflection density
US4529319A (en) Method and apparatus for the detection of thermo-optical signals
JPH08503767A (en) Device for qualitative and / or quantitative analysis of samples
JPH0650882A (en) Optical measuring device
KR950014849A (en) Photometric detectors scattered by thin films of colloidal media
EP0586054A1 (en) Spectroscopic imaging system using a pulsed electromagnetic radiation source and an interferometer
JPH06505092A (en) Qualitative and/or quantitative measurement device for analytical sample composition
JPH04301744A (en) Prism for micro-total refection measurement
JP4737896B2 (en) Sample concentration measuring device
EP0447991B1 (en) Apparatus for measuring the distribution of the size of diffraction-scattering type particles
EP0510175B1 (en) Fluorescence assay apparatus
JP2597515Y2 (en) Total reflection absorption spectrum measurement device
JPH11142241A (en) Measuring apparatus for spectral transmittance
JP2002357544A (en) Measuring apparatus
US5212393A (en) Sample cell for diffraction-scattering measurement of particle size distributions
JPH0712715A (en) Total reflection absorbing spectrum measuring device
SU819646A1 (en) Device for determination of diffusive media optical characteristics
JPH04138340A (en) Infrared spectrum measuring head and measuring apparatus
JPH049570Y2 (en)

Legal Events

Date Code Title Description
A01 Written decision to grant a patent or to grant a registration (utility model)

Free format text: JAPANESE INTERMEDIATE CODE: A01

Effective date: 20000202