JPH0862133A - Microscopic infrared spectrophotometer - Google Patents

Microscopic infrared spectrophotometer

Info

Publication number
JPH0862133A
JPH0862133A JP22251194A JP22251194A JPH0862133A JP H0862133 A JPH0862133 A JP H0862133A JP 22251194 A JP22251194 A JP 22251194A JP 22251194 A JP22251194 A JP 22251194A JP H0862133 A JPH0862133 A JP H0862133A
Authority
JP
Japan
Prior art keywords
infrared
sample
detector
spectrum
light source
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
JP22251194A
Other languages
Japanese (ja)
Other versions
JP2581016B2 (en
Inventor
Norinaga Sasaki
宣良 笹木
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.)
NEC Corp
Original Assignee
NEC 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 NEC Corp filed Critical NEC Corp
Priority to JP22251194A priority Critical patent/JP2581016B2/en
Publication of JPH0862133A publication Critical patent/JPH0862133A/en
Application granted granted Critical
Publication of JP2581016B2 publication Critical patent/JP2581016B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Landscapes

  • Investigating Or Analysing Materials By Optical Means (AREA)

Abstract

PURPOSE: To realize measurement of infrared absorption spectrum in a micro region using a nonlinear phenomenon. CONSTITUTION: A variable wavelength infrared laser beam from a light source 1 is projected to a sample and the transmitted infrared beam 4 impinges on a crystal 5 of nonlinear material. A second or third harmonic 6 emitted therefrom is restricted by means of an aperture 8. Consequently, an IR spectrum can be measured for a micro region smaller by a factor of 2 or 3 as compared with a conventional region.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は顕微赤外分光光度計に関
し、特に微小領域の赤外線吸収スペクトルの測定が可能
な顕微赤外分光光度計に関するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a micro-infrared spectrophotometer, and more particularly to a micro-infrared spectrophotometer capable of measuring an infrared absorption spectrum in a minute area.

【0002】[0002]

【従来の技術】図2に従来の微小領域の赤外吸収スペク
トル(以下、IRスペクトルと略す。)の測定法の概略
を透過法を例として示す。微小領域のIRスペクトル
は、白色光源21から出射された2.5〜25μmの波
長をもつ赤外ビーム22をある程度収束し、試料23に
透過させて試料の情報を含ませ、該情報を含む赤外ビー
ム24のうち観測対象領域以外の情報をもつ赤外ビーム
をアパーチャ26で除外し、観察対象領域のビーム27
のみを検出器28で検出し、電気信号に変換してデータ
処理装置29に送り、IRスペクトルに変換することに
より得られる。
2. Description of the Related Art FIG. 2 shows an outline of a conventional method for measuring an infrared absorption spectrum (hereinafter abbreviated as IR spectrum) of a minute region, using a transmission method as an example. The IR spectrum of the minute region converges the infrared beam 22 having a wavelength of 2.5 to 25 μm emitted from the white light source 21 to some extent, transmits the infrared beam 22 to the sample 23, and includes the information of the sample. The infrared beam having the information other than the observation target area is excluded from the outer beam 24 by the aperture 26, and the beam 27 of the observation target area is removed.
It is obtained by detecting only the light with the detector 28, converting it into an electric signal and sending it to the data processor 29, and converting it into an IR spectrum.

【0003】[0003]

【発明が解決しようとする課題】アパーチャで絞ること
のできる赤外ビーム径の限界はビームの波長に依存し、
10μmの波長をもつビームであれば、10μmφ以下
に絞ることは困難である。有用なIRスペクトルを得る
には、少なくとも2.5〜14μmの波長領域で連続的
な波長をもつ赤外ビームが必要で、この場合、アパーチ
ャで絞れるビーム径の限界は約14μmφとなる。従っ
て、それ以下の領域のIRスペクトルを得ることはでき
ないという問題点があった。本発明の目的は、このよう
な従来の問題点を解決することにある。
The limit of the diameter of the infrared beam that can be narrowed by the aperture depends on the wavelength of the beam.
If the beam has a wavelength of 10 μm, it is difficult to narrow the beam to 10 μmφ or less. In order to obtain a useful IR spectrum, an infrared beam having a continuous wavelength in the wavelength region of at least 2.5 to 14 μm is required, and in this case, the beam diameter that can be narrowed by the aperture is limited to about 14 μmφ. Therefore, there is a problem that an IR spectrum in a region smaller than that cannot be obtained. An object of the present invention is to solve such conventional problems.

【0004】[0004]

【課題を解決するための手段】本発明は、試料にコヒー
レントな赤外光を照射する赤外光光源と、前記試料を透
過した透過赤外ビームを検出する検出器と、前記試料と
前記検出器との間に配置され、前記透過赤外ビームを入
射して2次または3次高調波とする非線形光学材料の結
晶と、前記非線形光学材料結晶の検出器側に配置され
て、前記2次または3次高長波を絞り込むアパーチャと
を備えてなることを特徴とする顕微赤外分光光度計であ
る。ここで、赤外光光源としては、波長可変赤外線レー
ザがあげられる。
SUMMARY OF THE INVENTION The present invention provides an infrared light source for irradiating a sample with coherent infrared light, a detector for detecting a transmitted infrared beam transmitted through the sample, and a detector for detecting the transmitted infrared beam. A nonlinear optical material crystal, which is disposed between the nonlinear optical material crystal and a second or third harmonic by making the transmitted infrared beam incident thereon, Or, an aperture for narrowing down a third-order high-long wave is provided. Here, as the infrared light source, a variable wavelength infrared laser can be used.

【0005】[0005]

【作用】本発明は、波長可変赤外線レーザ等のコヒーレ
ントな光源をもち、非線形光学材料の結晶をアパーチャ
の前に設置し、試料の情報を含んだ赤外ビームを透過さ
せ、そこから得られる波長が1/2の2次高調波、また
は1/3の3次高調波をアパーチャで絞ることで、絞れ
るビーム径の限界を従来の1/2〜1/3に向上させ、
この微小領域のIRスペクトルの測定を可能とするもの
である。
According to the present invention, a coherent light source such as a wavelength-tunable infrared laser is provided, a crystal of a nonlinear optical material is set in front of an aperture, an infrared beam containing information on a sample is transmitted, and a wavelength obtained therefrom is obtained. By narrowing the second harmonic of 1/2 or the third harmonic of 1/3 with an aperture, the limit of the beam diameter that can be narrowed is improved to 1/2 to 1/3 of the conventional one,
The IR spectrum of this minute region can be measured.

【0006】[0006]

【実施例】次に本発明の実施例について、透過法の場合
を例とし、図1を参照して示す。本装置は、コヒーレン
トな赤外ビーム2を試料3に照射する光源1と、試料3
の検出器側に配置された非線形光学材料よりなる結晶5
と、この非線形光学材料の結晶5の検出器側に配置され
たアパーチャ8および検出器10を含む。光源1から出
たコヒーレントな赤外ビーム2は試料3を透過し、試料
の情報を含む。この試料の情報を含む赤外ビーム4が非
線形光学材料の結晶5を透過したとき、2次または3次
高調波6が得られる。この2次または3次高調波6の波
長は、赤外ビーム2および4の1/2または1/3にな
っている。この2次または3次高調波6の観測対象領域
以外をアパーチャ8で除外し、観測対象領域のビーム9
のみを検出器10へと導く。観測対象領域のビーム9は
検出器10で電気信号に変換されデータ処理装置11へ
送られ、IRスペクトルへ変換される。
EXAMPLES Next, examples of the present invention will be described with reference to FIG. 1, taking the case of the transmission method as an example. The apparatus comprises a light source 1 for irradiating a coherent infrared beam 2 to a sample 3 and a sample 3
Crystal 5 made of nonlinear optical material arranged on the detector side of
And an aperture 8 and a detector 10 arranged on the detector side of the crystal 5 of this nonlinear optical material. The coherent infrared beam 2 emitted from the light source 1 passes through the sample 3 and contains information on the sample. When the infrared beam 4 containing the information of this sample passes through the crystal 5 of the nonlinear optical material, the second or third harmonic wave 6 is obtained. The wavelength of the second or third harmonic 6 is 1/2 or 1/3 of the infrared beams 2 and 4. The area other than the observation area of the second or third harmonic 6 is excluded by the aperture 8 and the beam 9 of the observation area is removed.
Only lead to the detector 10. The beam 9 in the observation target area is converted into an electric signal by the detector 10 and sent to the data processing device 11 to be converted into an IR spectrum.

【0007】非線形現象を利用するためには、コヒーレ
ントな光を非線形光学材料の結晶に入射しなくてはなら
ない。また、IRスペクトルを得るには、2.5〜14
μmの波長領域をもつ赤外ビームを試料に照射する必要
がある。したがって、本発明においては、光源1に波長
可変赤外線レーザ等を用い、2.5〜14μmの波長領
域を連続的に掃引する。これにより、非線形光学材料の
結晶5を透過したときに得られる2次または3次高調波
の波長は、1.25〜7μm、または0.83〜4.6
7μmとなり、アパーチャ8により絞れる限界が、従来
の14μmφから、7μmφまたは4.67μmφへと
向上し、IRスペクトルを得ることのできる試料領域
が、従来の14μmφから、7μmφまたは4.67μ
mφへと狭くなり、より狭い領域のIRスペクトルを得
ることが可能となる。
In order to utilize the nonlinear phenomenon, coherent light must be incident on the crystal of the nonlinear optical material. Moreover, in order to obtain an IR spectrum, 2.5 to 14
It is necessary to irradiate the sample with an infrared beam having a wavelength range of μm. Therefore, in the present invention, a variable wavelength infrared laser or the like is used as the light source 1, and the wavelength region of 2.5 to 14 μm is continuously swept. Thereby, the wavelength of the second or third harmonic obtained when the light passes through the crystal 5 of the nonlinear optical material is 1.25 to 7 μm, or 0.83 to 4.6.
7 μm, the limit that can be narrowed down by the aperture 8 is improved from 14 μmφ of the past to 7 μmφ or 4.67 μmφ, and the sample region where the IR spectrum can be obtained is from 7 μmφ of the conventional 14 μmφ or 4.67 μm
mφ, and an IR spectrum in a narrower region can be obtained.

【0008】[0008]

【発明の効果】以上説明したように、本発明によれば従
来の1/2〜1/3の微小領域のIRスペクトル測定が
可能となる。
As described above, according to the present invention, it is possible to measure the IR spectrum in a minute region of 1/2 to 1/3 of the conventional one.

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

【図1】本発明による顕微赤外分光光度計の一実施例の
構成図である。
FIG. 1 is a configuration diagram of an embodiment of a microscopic infrared spectrophotometer according to the present invention.

【図2】従来例による顕微赤外分光光度計の一例の構成
図である。
FIG. 2 is a configuration diagram of an example of a conventional microscopic infrared spectrophotometer.

【符号の説明】[Explanation of symbols]

1 光源 2 赤外ビーム 3 試料 4 試料の情報を含む赤外ビーム 5 非線形光学材料の結晶 6 2次または3次高調波 8 アパーチャ 9 観察対象領域のビーム 10 検出器 11 データ処理装置 21 光源 22 赤外ビーム 23 試料 24 試料の情報を含む赤外ビーム 26 アパーチャ 27 観察対象領域のビーム 28 検出器 29 データ処理装置 Reference Signs List 1 light source 2 infrared beam 3 sample 4 infrared beam containing information of sample 5 crystal of nonlinear optical material 6 second or third harmonic 8 aperture 9 beam in observation target area 10 detector 11 data processing device 21 light source 22 red External beam 23 Sample 24 Infrared beam including information of the sample 26 Aperture 27 Beam in observation area 28 Detector 29 Data processing device

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】 試料にコヒーレントな赤外光を照射する
赤外光光源と、前記試料を透過した透過赤外ビームを検
出する検出器と、前記試料と前記検出器との間に配置さ
れ、前記透過赤外ビームを入射して2次または3次高調
波とする非線形光学材料の結晶と、前記非線形光学材料
結晶の検出器側に配置されて、前記2次または3次高調
波を絞り込むアパーチャとを備えてなることを特徴とす
る顕微赤外分光光度計。
1. An infrared light source for irradiating a sample with coherent infrared light, a detector for detecting a transmitted infrared beam transmitted through the sample, and a detector arranged between the sample and the detector, A crystal of a nonlinear optical material that makes the transmitted infrared beam incident into a second or third harmonic, and an aperture arranged on the detector side of the nonlinear optical material to narrow down the second or third harmonic. And a microscopic infrared spectrophotometer.
【請求項2】 赤外光光源が波長可変赤外線レーザであ
る請求項1記載の顕微赤外分光光度計。
2. The microscopic infrared spectrophotometer according to claim 1, wherein the infrared light source is a tunable infrared laser.
JP22251194A 1994-08-24 1994-08-24 Microscopic infrared spectrophotometer Expired - Fee Related JP2581016B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP22251194A JP2581016B2 (en) 1994-08-24 1994-08-24 Microscopic infrared spectrophotometer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP22251194A JP2581016B2 (en) 1994-08-24 1994-08-24 Microscopic infrared spectrophotometer

Publications (2)

Publication Number Publication Date
JPH0862133A true JPH0862133A (en) 1996-03-08
JP2581016B2 JP2581016B2 (en) 1997-02-12

Family

ID=16783583

Family Applications (1)

Application Number Title Priority Date Filing Date
JP22251194A Expired - Fee Related JP2581016B2 (en) 1994-08-24 1994-08-24 Microscopic infrared spectrophotometer

Country Status (1)

Country Link
JP (1) JP2581016B2 (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB2312805A (en) * 1996-05-03 1997-11-05 Yeda Res & Dev Scanning laser microscopy using only 3rd harmonics
KR101487812B1 (en) * 2013-06-07 2015-01-30 한국과학기술연구원 Device for extracting depth information using infrared light and Method thereof
GB2624663A (en) * 2022-11-24 2024-05-29 Univ Nottingham Trent A frequency conversion device for use with an infrared imaging system

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB2312805A (en) * 1996-05-03 1997-11-05 Yeda Res & Dev Scanning laser microscopy using only 3rd harmonics
US5828459A (en) * 1996-05-03 1998-10-27 Yeda Research And Development Co. Ltd. Apparatus and method for scanning laser microscopy
GB2312805B (en) * 1996-05-03 2000-06-21 Yeda Res & Dev Apparatus and method for scanning laser microscopy
DE19718909B4 (en) * 1996-05-03 2004-04-08 Yeda Research And Development Co., Ltd. Device and method for scanning laser microscopy
KR101487812B1 (en) * 2013-06-07 2015-01-30 한국과학기술연구원 Device for extracting depth information using infrared light and Method thereof
GB2624663A (en) * 2022-11-24 2024-05-29 Univ Nottingham Trent A frequency conversion device for use with an infrared imaging system

Also Published As

Publication number Publication date
JP2581016B2 (en) 1997-02-12

Similar Documents

Publication Publication Date Title
US6839496B1 (en) Optical fibre probe for photoacoustic material analysis
US3556659A (en) Laser-excited raman spectrometer
US4415265A (en) Method and apparatus for aerosol particle absorption spectroscopy
EP0056239A1 (en) Method of measuring Raman spectra and laser Raman spectrophotometry system
US5469255A (en) Method and apparatus for spectrometric measurement of particulate surfaces
US5406377A (en) Spectroscopic imaging system using a pulsed electromagnetic radiation source and an interferometer
JP2581016B2 (en) Microscopic infrared spectrophotometer
JPH1189799A (en) Concentration measuring device for specified ingredient
JPH0610636B2 (en) Gas spectroscope
JP7486178B2 (en) Spectroscopic equipment
US4035080A (en) Apparatus of spectroscopy of scattering light
US3932762A (en) Apparatus for measuring radiation angle dependence
JPS60159619A (en) Picture monochromator
JPH10153561A (en) Photothermal transduction spectral analyzer
JPH03148043A (en) Spectroscopic measuring apparatus using infrared-ray microscope method
JPH11142241A (en) Measuring apparatus for spectral transmittance
JPH102803A (en) Optical device
JPH11326205A (en) Laser breakdown spectroscopic analyzer
JP3385670B2 (en) Infrared spectrophotometer
JPH08233728A (en) Microscopic total reflection absorption spectrum measuring apparatus
JPS6281550A (en) Photoacoustic spectroscope
JP2943236B2 (en) Total reflection absorption spectrum measurement device
JP3440273B2 (en) Nonlinear susceptibility spectrum measuring method and device
JP2006064399A (en) Breakage location detecting apparatus and fracture location detecting method of optical fiber
GB2275348A (en) Optical fibre probe

Legal Events

Date Code Title Description
LAPS Cancellation because of no payment of annual fees