JP3039569B2 - Prism for total internal reflection measurement - Google Patents

Prism for total internal reflection measurement

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Publication number
JP3039569B2
JP3039569B2 JP9129491A JP9129491A JP3039569B2 JP 3039569 B2 JP3039569 B2 JP 3039569B2 JP 9129491 A JP9129491 A JP 9129491A JP 9129491 A JP9129491 A JP 9129491A JP 3039569 B2 JP3039569 B2 JP 3039569B2
Authority
JP
Japan
Prior art keywords
reflecting surface
incident
sample
light
reflecting
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
JP9129491A
Other languages
Japanese (ja)
Other versions
JPH04301744A (en
Inventor
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

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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 total reflection measurement suitable for a microscopic system for qualitative analysis by irradiating a minute area of a sample with light.

【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。
2. Description of the Related Art In a total reflection measurement of a minute sample, light from a light source is narrowed down by a beam condenser and made incident on a prism on which the sample is adhered, and light absorbed by the sample is detected. However, since the light beam incident on the prism is diffused in the prism,
There is a problem that the measurement results for the entire sample cannot be obtained and analysis that specifies a minute area of the sample cannot be performed. In order to solve such a problem, a prism formed in a cross-shaped “<” shape is used, and a sample is brought into close contact with the prism for measurement. According to this method, it is possible to select a portion to be irradiated with infrared rays. On the other hand, in addition to the problem of requiring four times of total reflection before emission, the optical path length is inevitably increased and attenuation is caused. However, application to a sample having a high refractive index such as carbon is difficult.

【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。
SUMMARY OF THE INVENTION The present invention has been made in view of the above circumstances, and an object of the present invention is to specify a measurement area of a sample, and to further specify an optical path length from incidence to emission. It is an object of the present invention to provide a novel prism for measuring total internal reflection, which makes it possible to reduce the attenuation by reducing the angle of incidence, and to make it possible to perform measurement at a plurality of large and small incident angles with 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、入射面と出射面とが対向す
るように形成され、前記入射面からの入射光に対して全
反射する第1の反射面と、第1の反射面に対向するとと
もに全反射する第2の反射面と、第2の反射面に対向す
るとともに第1の反射面に隣接する側に前記出射面に対
して全反射する第3の反射面とを備え、第1、第2、第
3の反射面のいずれをも試料当接面とするようにした。
In order to solve such a problem, according to the present invention, an incident surface and an outgoing surface are formed so as to face each other, and the incident light from the incident surface is totally reflected. A first reflecting surface, a second reflecting surface facing the first reflecting surface and totally reflecting the light, and a second reflecting surface facing the second reflecting surface and adjacent to the first reflecting surface. A third reflecting surface for total reflection of the first, second,
Each of the three reflecting surfaces was used as a sample contact surface .

【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。
The first and third reflecting surfaces receive light at a relatively large incident angle with respect to incident light, and the second reflecting surface receives light at a relatively small incident angle. When the sample is brought into close contact with and fixed to the third reflecting surface, measurement with a relatively large incident angle becomes possible. When the sample is brought into close contact with and fixed to the first reflecting surface, measurement with a relatively small incident angle becomes possible. In addition, by changing the position where the light from the light source is incident, part of the light does not reach the third reflecting surface and does not enter the detector, so that it is possible to perform measurement while selecting the sample area. 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 described below with reference to the illustrated embodiments. FIG. 1 shows an embodiment of the present invention. In the drawing, reference numeral 1 denotes an M-shaped cross section made of an optical material capable of transmitting infrared rays, for example, KRS-5, ZnSe, or ZnS. In the infrared micro total reflection measurement prism, a first reflection surface 3 is formed at an angle at which total reflection is performed on infrared light incident on the incident surface 2. The reflecting surface 3 has a reflecting surface set at an angle of 30 degrees with respect to the incident surface 2 so that infrared light is incident at an angle of 60 degrees. On the side opposite to the first reflecting surface 3, the second angle is perpendicular to the incident surface 2 and is an angle for totally reflecting infrared rays from the first reflecting surface 3, for example, an incident angle of 45 degrees. On the side adjacent to the first reflecting surface 3 is formed a reflecting surface 4 at which the infrared light reflected by the second reflecting surface 4 is totally reflected with respect to the emitting surface 6, for example, an incident angle of 60 degrees. The third reflecting surface 5 is formed so as 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 requiring a relatively small incident angle, the sample S 1 is brought into close contact with the first reflection surface 2 as shown in FIG. Fix it. In this state, the infrared light incident from the incident surface 2 is reflected by the first reflecting surface 3 and is incident on the second reflecting surface 4 at a relatively small incident angle of about 45 degrees. This allows the second
An infrared ray enters the sample S1 fixed at a relatively small angle on the reflecting surface 4 of the third reflecting surface 4 so as to absorb a component having a wavelength corresponding to the characteristics of the sample, and reflect other wavelength components to form a third reflecting surface. The light is reflected by 5 and exits from the exit surface 6. As a result, a total reflection measurement of a sample that requires the incidence of infrared light at a relatively small incident angle is 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 a measurement at a large incident angle is required, the sample S is brought into close contact with and fixed to the first reflecting surface 3 as shown in FIG. because they have a relatively large incident angle with respect to, will be incident at a large incident angle of 60 degrees to the sample S 2. Some of the wavelength components are absorbed according to the characteristics of the sample, and
Are reflected by the reflection surface 4 and the third reflection surface 5 and are emitted to the outside from the emission surface. As shown in FIG. 3 (c), by attaching and fixing the sample to the plurality of reflection surfaces 3 and 5, the sample can be subjected to multiple times of absorption and measurement with high sensitivity is possible.

【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 reflecting surface, the position on the incident surface 2 where the light beam from the light source is incident is shifted as shown in FIG. Part of the infrared light reflected by the second reflecting surface 4 does not reach the third reflecting surface 5 and does not enter the detector. As a result, it is possible to perform measurement in which the region of the sample is specified.

【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。
In this embodiment, an example of measurement using infrared light has been described. However, it is apparent that the present invention can be applied to analysis using visible light by using a visible light transmitting material.

【0011】[0011]

【発明の効果】以上説明したように本発明においては、
入射面と出射面とが対向するように形成され、入射面か
らの入射光に対して全反射する第1の反射面と、第1の
反射面に対向するとともに全反射する第2の反射面と、
第2の反射面に対向するとともに第1の反射面に隣接す
る側に出射面に対して全反射する第3の反射面とを備
え、第1、第2、第3の反射面のいずれをも試料の当接
面としたので、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の反射面に試料を当接させると、比較的大きな入射
角による測定が、また第2の反射面に試料を当接させる
、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3つの面のいずれを選択するかにより試料
への入射角を変更することができる。さらに光源からの
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。
As described above, in the present invention,
A first reflecting surface which is formed so that the incident surface and the emitting surface face each other and totally reflects the incident light from the incident surface; and a second reflecting surface which faces the first reflecting surface and totally reflects the light. When,
A third reflecting surface that faces the second reflecting surface and that is totally reflected on the exit surface on a side adjacent to the first reflecting surface; and any one of the first, second, and third reflecting surfaces is provided. Contact of sample
Having a surface, because the reflection surface of the first or third light is incident at a relatively large angle of incidence with respect to the incident light, and the second reflecting surface the light is incident at relatively small angles of incidence, First,
When the sample is brought into contact with the third reflecting surface, measurement at a relatively large incident angle is performed, and the sample is brought into contact with the second reflecting surface .
Thus, the measurement can be performed with a relatively small incident angle, and the incident angle to the sample can be changed by selecting one of the three surfaces on which the sample is mounted. Further, by changing the position where the light from the light source is incident, a part of the light does not reach the third reflecting surface and does not enter the detector, so that the measurement can be performed while selecting the sample area.

【図面の簡単な説明】[Brief description of the 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 an 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。
FIGS. 2A, 2B, and 2C are explanatory views showing states of use of the prism.

【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 an operation when a specific region of a sample is selected and measured.

【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Reference Signs List 1 prism main body 2 entrance surface 3 first reflection surface 4 second reflection surface 5 third reflection surface 6 exit surface S 1 , S 2 sample

Claims (1)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】 入射面と出射面とが対向するように形成
され、前記入射面からの入射光に対して全反射する第1
の反射面と、第1の反射面に対向するとともに全反射す
る第2の反射面と、第2の反射面に対向するとともに第
1の反射面に隣接する側に前記出射面に対して全反射す
る第3の反射面とを備え、第1、第2、第3の反射面の
いずれをも試料当接面とする顕微全反射測定用プリズ
ム。
A first surface which is formed so that an incident surface and an outgoing surface face each other, and which is totally reflected with respect to incident light from the incident surface;
A second reflecting surface facing the first reflecting surface and totally reflecting, and a second reflecting surface facing the second reflecting surface and adjacent to the first reflecting surface with respect to the emission surface. A third reflecting surface that reflects the light, and the first, second, and third reflecting surfaces
All are prisms for measuring total internal reflection with a sample contact 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 JPH04301744A (en) 1992-10-26
JP3039569B2 true 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
JP3201135U (en) * 2014-09-10 2015-11-19 余志雄Yu Chih Hsiung Assembly shelf coupler

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP4800244B2 (en) * 2007-03-13 2011-10-26 浜松ホトニクス株式会社 Terahertz wave measuring device

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP3201135U (en) * 2014-09-10 2015-11-19 余志雄Yu Chih Hsiung Assembly shelf coupler

Also Published As

Publication number Publication date
JPH04301744A (en) 1992-10-26

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