JPH0465336B2 - - Google Patents
Info
- Publication number
- JPH0465336B2 JPH0465336B2 JP57174529A JP17452982A JPH0465336B2 JP H0465336 B2 JPH0465336 B2 JP H0465336B2 JP 57174529 A JP57174529 A JP 57174529A JP 17452982 A JP17452982 A JP 17452982A JP H0465336 B2 JPH0465336 B2 JP H0465336B2
- Authority
- JP
- Japan
- Prior art keywords
- laser
- sample
- raman
- light
- objective lens
- 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
Links
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/62—Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light
- G01N21/63—Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light optically excited
- G01N21/65—Raman scattering
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/62—Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light
- G01N21/63—Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light optically excited
- G01N21/65—Raman scattering
- G01N2021/653—Coherent methods [CARS]
- G01N2021/656—Raman microprobe
Landscapes
- Health & Medical Sciences (AREA)
- Nuclear Medicine, Radiotherapy & Molecular Imaging (AREA)
- Physics & Mathematics (AREA)
- Life Sciences & Earth Sciences (AREA)
- Chemical & Material Sciences (AREA)
- Analytical Chemistry (AREA)
- Biochemistry (AREA)
- General Health & Medical Sciences (AREA)
- General Physics & Mathematics (AREA)
- Immunology (AREA)
- Pathology (AREA)
- Investigating, Analyzing Materials By Fluorescence Or Luminescence (AREA)
Description
【発明の詳細な説明】
本発明は、レーザ光源と、該レーザ光源からの
レーザ光の進路を半透鏡によつて90°曲げ、対物
レンズを経て試料に照射し、かつレーザ光照射に
よつて前記試料から発生したラマン散乱光を前記
対物レンズで集光し、さらに前記半透鏡を経て試
料と対物レンズのなす光軸方向に取り出す光学顕
微鏡と、該光学顕微鏡から取り出されたラマン散
乱光を分光、検出するためのラマン分光光度計と
よりなるレーザ・ラマン・マイクロプローブに関
する。DETAILED DESCRIPTION OF THE INVENTION The present invention includes a laser light source, a laser light beam from the laser light source whose path is bent by 90° using a semi-transparent mirror, and a sample is irradiated through an objective lens, and the laser light irradiation path is bent by 90°. An optical microscope that collects the Raman scattered light generated from the sample with the objective lens and further extracts it in the direction of the optical axis formed by the sample and the objective lens through the semi-transparent mirror, and spectroscopy the Raman scattered light extracted from the optical microscope. , a laser Raman microprobe consisting of a Raman spectrophotometer for detection.
従来の光学顕微鏡をレーザ光照射、ラマン散乱
光集光に用いるレーザ・ラマン・マイクロプロー
ブにおいては、レーザ光を半透鏡で90°方向に曲
げ、対物レンズを経て試料に照射し、同じ対物レ
ンズでラマン散乱光を集光し、半透鏡を経てラマ
ン散乱光を取り出す構造のため、試料からのレー
ザ反射光とラマン散乱光は同一光路を通る。この
ため試料の状態変化やレーザ照射点のずれをモニ
タするには半透鏡を経て取り出されるレーザ反射
光およびラマン散乱光の一部をビーム・スプリツ
タ等で分割して取り出しプロジエクタ、テレビカ
メラなどで顕微鏡像を観察するが、ラマン分光光
度計へ導入するラマン散乱光量がモニタ用に分割
した分だけ減少するため、検出感度が低下する欠
点があつた。またラマン分光光度計へはレーザ反
射光もラマン散乱光と同一光路を通つて同時に導
入されるため、分光光度計内で迷光となり、特に
レーザ波長に近い低波数領域でのラマン散乱光測
定の妨害が著しい欠点があつた。 In the laser Raman microprobe, which uses a conventional optical microscope to irradiate laser light and focus Raman scattered light, the laser light is bent in a 90° direction with a semi-transparent mirror, and then irradiated onto the sample through an objective lens. Because the structure is such that the Raman scattered light is collected and extracted through a semi-transparent mirror, the laser reflected light from the sample and the Raman scattered light pass through the same optical path. Therefore, in order to monitor changes in the state of the sample and shifts in the laser irradiation point, a portion of the laser reflected light and Raman scattered light extracted through the semi-transparent mirror is split using a beam splitter, etc., and then taken out using a microscope using a projector, TV camera, etc. The image is observed, but since the amount of Raman scattered light introduced into the Raman spectrophotometer is reduced by the amount divided for monitoring, there is a drawback that detection sensitivity is reduced. In addition, since the laser reflected light is simultaneously introduced into the Raman spectrophotometer through the same optical path as the Raman scattered light, it becomes stray light within the spectrophotometer, interfering with Raman scattered light measurements, especially in the low wavenumber region near the laser wavelength. However, there were significant drawbacks.
本発明の目的は、上記した従来技術の欠点をな
くし、ラマン散乱光測定時ラマン散乱光の損失が
少ない状態で常時試料状態のモニタができかつ、
レーザ反射光に基づく分光光度計内での迷光を減
少できるレーザ・ラマン・マイクロプローブを提
供することにある。 An object of the present invention is to eliminate the drawbacks of the prior art described above, to constantly monitor the state of a sample with little loss of Raman scattered light during Raman scattered light measurement, and to
An object of the present invention is to provide a laser Raman microprobe that can reduce stray light within a spectrophotometer based on laser reflected light.
上記目的を達成するために、本発明による冒頭
に述べた種類のレーザ・ラマン・マイクロプロー
ブは、試料と対物レンズのなす光軸上の半透鏡後
方に、前記光軸に対し所定の角度をなすように設
けられ、レーザ発振波長のみを透過し、レーザ発
振波長より長波長の光を反射するダイクロイツ
ク・ミラーと、該ダイクロイツク・ミラー後方に
設けられたレーザ波長での顕微鏡像モニタとから
なる試料モニタを備えることを要旨とする。すな
わち、本発明では対物レンズで集光され、半透鏡
を経て取り出したレーザ反射光とラマン散乱光
を、レーザ反射光を透過し、レーザ反射光より長
波長のラマン散乱光を反射するダイクロイツク・
ミラーによつてラマン散乱光の進路を変えること
により分割して別々に取り出し、レーザ反射光光
路上に配置されたレーザ波長での顕微鏡像モニタ
によりラマン散乱光測定中試料状態を観察すると
ともに、レーザ反射光の混入しないラマン散乱光
を効率よく分光光度計に導入する。 In order to achieve the above object, the laser Raman microprobe of the type mentioned at the beginning according to the present invention is provided with a laser Raman microprobe of the type mentioned at the beginning, which is arranged behind a semi-transparent mirror on the optical axis formed by the sample and the objective lens, and which forms a predetermined angle with respect to the optical axis. It consists of a dichroic mirror that transmits only the laser oscillation wavelength and reflects light with a wavelength longer than the laser oscillation wavelength, and a microscope image monitor at the laser wavelength that is provided behind the dichroic mirror. The main point is to be equipped with a sample monitor. That is, in the present invention, the laser reflected light and the Raman scattered light are collected by an objective lens and taken out through a semi-transparent mirror.
By changing the path of the Raman scattered light using a mirror, the Raman scattered light is divided and taken out separately, and the state of the sample is observed during the Raman scattered light measurement using a microscope image monitor at the laser wavelength placed on the laser reflected light optical path. To efficiently introduce Raman scattered light without mixing reflected light into a spectrophotometer.
以下に、附図を参照しながら、実施例を用いて
本発明を一層詳細に説明するが、それらは例示に
過ぎず、本発明の枠を越えることなしにいろいろ
な改良や変形があり得ることは勿論である。 Hereinafter, the present invention will be explained in more detail using examples with reference to the accompanying drawings, but these are merely illustrative and it is understood that various improvements and modifications may be made without going beyond the scope of the present invention. Of course.
第1図において、ラマン散乱光励起用レーザ光
1は集光レンズ2を経て顕微鏡の半透鏡3に入射
する。半透鏡3で入射方向に対し90°曲げられた
レーザ光は対物レンズ4により試料5の上に焦点
を結ぶ。試料5から発生したレーザ反射光6およ
びラマン散乱光7は対物レンズ4によつて集光さ
れ、半透鏡3を経て対物レンズ4と半透鏡3のな
す光軸に対し45°の角をなすように配置されたダ
イクロイツク・ミラー8に入射する。ダイクロイ
ツク・ミラー8の特性によつて、透過したレーザ
反射光は減光フイルタ9、集光レンズ10を経て
レーザ反射光による顕微鏡像モニタ11に入射
し、試料状態をモニタする。またダイクロイツ
ク・ミラー8の特性によつて対物レンズ4と半透
鏡3のなす光軸に対し90°方向に曲げられたラマ
ン散乱光は集光レンズ12を経て分光光度計入射
スリツト13上に結像する。 In FIG. 1, a laser beam 1 for excitation of Raman scattered light enters a semi-transparent mirror 3 of a microscope through a condensing lens 2. The laser beam is bent by 90 degrees with respect to the incident direction by the semi-transparent mirror 3 and is focused onto the sample 5 by the objective lens 4. The laser reflected light 6 and the Raman scattered light 7 generated from the sample 5 are focused by the objective lens 4 and passed through the semi-transparent mirror 3 so that they form an angle of 45° with respect to the optical axis formed by the objective lens 4 and the semi-transparent mirror 3. The light is incident on a dichroic mirror 8 located at . Due to the characteristics of the dichroic mirror 8, the transmitted laser reflected light passes through a neutral density filter 9 and a condensing lens 10, and enters a microscope image monitor 11 using laser reflected light to monitor the state of the sample. Furthermore, due to the characteristics of the dichroic mirror 8, the Raman scattered light is bent at 90 degrees with respect to the optical axis formed by the objective lens 4 and the semi-transparent mirror 3, and is focused onto the spectrophotometer entrance slit 13 through the condensing lens 12. Image.
このように構成することによつて、顕微鏡を用
いたレーザ・ラマン・マイクロプローブにおい
て、ラマン散乱光測定時の試料状態の同時モニタ
をする場合でも、ラマン散乱光の損失を少なくで
き、また同時に分光光度計内で迷光の原因となる
レーザ反射光を除去できる効果がある。 With this configuration, the loss of Raman scattered light can be reduced even when the sample condition is simultaneously monitored during Raman scattered light measurement using a laser, Raman, or microprobe using a microscope. This has the effect of eliminating laser reflected light that causes stray light within the photometer.
以上説明した通り、本発明によれば、試料の検
出感度を損なうことなく測定中の試料状態のモニ
タが可能となり、試料の状態変化、照射点のずれ
などを迅速に知ることができ、また特にレーザ波
長に近い低波数領域でのラマン散乱光の測定が感
度良く、容易に行なえるという利点が得られる。 As explained above, according to the present invention, it is possible to monitor the state of the sample during measurement without impairing the detection sensitivity of the sample, and it is possible to quickly find out changes in the state of the sample, shifts in the irradiation point, etc. This method has the advantage of being sensitive and easy to measure Raman scattered light in a low wavenumber region close to the laser wavelength.
図は本発明によるレーザ・ラマン・マイクロプ
ローブを模式的に示す構成図である。
1……ラマン散乱光励起用レーザ光、2……集
光レンズ、3……半透鏡、4……対物レンズ、5
……試料、6……レーザ反射光、7……ラマン散
乱光、8……ダイクロイツク・ミラー、9……減
光フイルタ、10……集光レンズ、11……レー
ザ反射光による顕微鏡像モニタ、12……集光レ
ンズ、13……分光光度計入射スリツト。
The figure is a configuration diagram schematically showing a laser Raman microprobe according to the present invention. DESCRIPTION OF SYMBOLS 1...Raman scattered light excitation laser beam, 2...Condensing lens, 3...Semi-transparent mirror, 4...Objective lens, 5
... Sample, 6 ... Laser reflected light, 7 ... Raman scattered light, 8 ... Dichroic mirror, 9 ... Attenuation filter, 10 ... Condenser lens, 11 ... Microscope image monitor using laser reflected light , 12...Condensing lens, 13...Spectrophotometer entrance slit.
Claims (1)
の進路を半透鏡によつて90°曲げ、対物レンズを
経て試料に照射し、かつレーザ光照射によつて前
記試料から発生したラマン散乱光を前記対物レン
ズで集光し、さらに前記半透鏡を経て試料と対物
レンズのなす光軸方向に取り出す光学顕微鏡と、
該光学顕微鏡から取り出されたラマン散乱光を分
光、検出するためのラマン分光光度計とよりなる
レーザ・ラマン・マイクロプローブにおいて、試
料と対物レンズのなす光軸上の半透鏡後方に、前
記光軸に対し所定の角度をなすように設けられ、
レーザ発振波長のみを透過し、レーザ発振波長よ
り長波長の光を前記ラマン分光光度計方向に反射
するダイクロイツク・ミラーと、光軸上の前記ダ
イクロイツク・ミラー後方に設けられたレーザ波
長での顕微鏡像モニタとからなる試料モニタを備
えることを特徴とするレーザ・ラマン・マイクロ
プローブ。1. A laser light source and the path of the laser light emitted from the laser light source are bent by 90° using a semi-transparent mirror, and the sample is irradiated through the objective lens, and the Raman scattered light generated from the sample by the laser light irradiation is an optical microscope that collects light with the objective lens and further extracts the light in the direction of the optical axis formed by the sample and the objective lens through the semi-transparent mirror;
In a laser Raman microprobe consisting of a Raman spectrophotometer for spectroscopy and detection of Raman scattered light extracted from the optical microscope, the optical axis is located behind the semi-transparent mirror on the optical axis formed by the sample and the objective lens. provided at a predetermined angle with respect to
a dichroic mirror that transmits only the laser oscillation wavelength and reflects light with a longer wavelength than the laser oscillation wavelength toward the Raman spectrophotometer; A laser Raman microprobe characterized by comprising a sample monitor consisting of a microscope image monitor.
Priority Applications (3)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP17452982A JPS5965242A (en) | 1982-10-06 | 1982-10-06 | Laser raman microprobe |
| US06/510,912 US4586819A (en) | 1982-07-09 | 1983-07-05 | Laser Raman microprobe |
| FR8311469A FR2530024B1 (en) | 1982-07-09 | 1983-07-08 | RAMAN LASER EFFECT MICROSOFT |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP17452982A JPS5965242A (en) | 1982-10-06 | 1982-10-06 | Laser raman microprobe |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5965242A JPS5965242A (en) | 1984-04-13 |
| JPH0465336B2 true JPH0465336B2 (en) | 1992-10-19 |
Family
ID=15980118
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP17452982A Granted JPS5965242A (en) | 1982-07-09 | 1982-10-06 | Laser raman microprobe |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5965242A (en) |
Family Cites Families (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| FR2253410A5 (en) * | 1973-12-03 | 1975-06-27 | Inst Nat Sante Rech Med | |
| JPS53135660A (en) * | 1977-04-30 | 1978-11-27 | Olympus Optical Co Ltd | Fluorescent photometric microscope using laser light |
-
1982
- 1982-10-06 JP JP17452982A patent/JPS5965242A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5965242A (en) | 1984-04-13 |
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