CN110006874A - A kind of coaxial femtosecond time Correlated Coherent anti-Stokes Raman scattering test macro - Google Patents

A kind of coaxial femtosecond time Correlated Coherent anti-Stokes Raman scattering test macro Download PDF

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CN110006874A
CN110006874A CN201910322121.0A CN201910322121A CN110006874A CN 110006874 A CN110006874 A CN 110006874A CN 201910322121 A CN201910322121 A CN 201910322121A CN 110006874 A CN110006874 A CN 110006874A
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pulse
femtosecond
femtosecond pulse
laser
coaxial
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CN110006874B (en
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王英惠
王文岩
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Jilin University
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Jilin University
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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N21/00Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
    • G01N21/62Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light
    • G01N21/63Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light optically excited
    • G01N21/65Raman scattering

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Abstract

The present invention relates to a kind of coaxial femtosecond time Correlated Coherent anti-Stokes Ramans to scatter test macro, belongs to ultrafast femtosecond laser field.It mainly include femtosecond pulse generator, optical parametric oscillator, reflecting mirror, beam splitter, dichroscope, annulus light generating device, sample cell, photomultiplier tube signal reception device and computer.The invention has the advantages that structure novel, the reflecting mirror that script is used to adjust angle between laser pulse is reduced to 2 by 6, pass through the change of the circle diameter to circular femto-second laser pulse, to adjust the angle between femto-second laser pulse, script is needed to the time correlation coherent anti-stokes raman scattering technology of 6 femto-second laser pulses adjusting freedom degrees, it is optimized for only adjusting 3 adjusting freedom degrees of circle diameter of 2 reflecting mirrors and circular femto-second laser pulse, substantially increases the stability, adjustable ease for use and repeatability of system.

Description

A kind of coaxial femtosecond time Correlated Coherent anti-Stokes Raman scattering test macro
Technical field
It is especially a kind of with good stability, adjustable ease for use the invention belongs to ultrafast femtosecond laser field, by The femto-second laser pulse that the circular femto-second laser pulse of a branch of Wavelength tunable and a branch of wavelength are fixed is coaxial come the one kind realized Femtosecond time Correlated Coherent anti-Stokes Raman scatters light test system.
Background technique
Time correlation coherent anti-stokes raman scattering technology is a kind of typical non-linear laser technology.Pass through change The characteristic of laser pulse makes time correlation coherent anti-stokes raman scattering technology have a variety of evolution forms, can visit Much information in sample ground state or excitation state.The development of nineteen sixties mid-term picosecond laser technology, 20 generation The appearance and the commercialization easy to operate of the early 1990s of the collision mode-locked dyelaser of discipline the seventies subpicosecond grade Self-locking mode is admired the succeeding in developing so that femtosecond laser technology is rapidly developed in different application field of sapphire laser.Its In, by the time correlation coherent anti-stokes raman scattering technology using femtosecond laser multi-pulse pumping, it can get many The important results such as structure of matter variation or energy conversion, people can have the substance and hair of the characteristics of luminescence using this technical research Photoreduction process, the flame temperature detection of fuel and identification of intermediate product etc..
Realization for time correlation coherent anti-stokes raman scattering technology needs to utilize three beams femtosecond laser arteries and veins Punching, wherein the wavelength of two beam femto-second laser pulses is identical, the wavelength and above-mentioned femtosecond of another beam femto-second laser pulse swash Light pulse wavelength is different, this three beams femto-second laser pulse needs converge in the same point of detected sample, and enter between them Relative angle when being mapped on sample needs to meet specific formula.This just needs to carry out the direction of three beams femto-second laser pulse It is accurate to adjust, in order to meet to three beams femto-second laser pulse can be adjusted per a branch of laser pulse its shooting angle and position this Experiment condition, each femto-second laser pulse require 2 reflecting mirrors of placement its angle to be adjusted, need 6 altogether Reflecting mirror.This significantly increases the difficulty and complexity of experimental implementation, and the repeatability of experiment is also poor.(Wang Yinghui two Ultrafast spectrum research [D] the Harbin Institute of Technology of the typical conjugatd polymers coherent vibrational process of kind, 2009.)
Summary of the invention
The present invention provides a kind of coaxial femtosecond time Correlated Coherent anti-Stokes Raman scattering test macro, to solve mesh Preceding existing because structure is complicated, significantly increases the difficulty and complexity of experimental implementation, the repeatability of experiment is also poor The problem of.
The technical solution adopted by the present invention is that: a branch of femtosecond pulse of femtosecond pulse generator generation, process After reflecting mirror one, beam splitter, femtosecond pulse is divided into the identical femtosecond pulse one of two beam wavelength and femtosecond pulse swashs Light two, wherein femtosecond pulse two enters optical parametric oscillator, the femtosecond pulse being emitted from optical parametric oscillator Three wavelength can change, and realize the adjusting of the wavelength of femtosecond pulse three in a certain range, shake by optical parameter The femtosecond pulse three for swinging device generation forms a branch of annulus shape femtosecond pulse and swashs after annulus light generating device Light, the annulus shape femtosecond pulse are closed at dichroscope with the femtosecond pulse one after the reflection of reflecting mirror two Beam, obtains that a branch of coaxial mixing femtosecond pulse, wherein femtosecond pulse one is located in circular femtosecond pulse Between;The coaxial mixing femtosecond pulse converges at the sample among sample cell after convex lens one, this is total at this time Sample among axis mixing femtosecond pulse and sample cell interacts, and generates a wavelength and converges on sample The different signal pulse laser of coaxial mixing femtosecond pulse, making the pulse laser through sample includes the femtosecond of three kinds of wavelength Pulse laser, annulus shape femtosecond pulse and signal pulse laser, the pulse laser comprising these three wavelength is by reflection After mirror three, optical filter, signal pulse laser is retained, and signal pulse laser passes through three shrink beam of convex lens, by photomultiplier transit Pipe reception device receives, and is recorded on the computer being connected with photomultiplier tube reception device.
The dichroscope reflects circular femtosecond pulse, transmits to femtosecond pulse one;
The annulus light generating device is expanded the concavees lens, convex lens and annulus light generating unit of part by femtosecond pulse The 0-2 π spiral phase plate composition divided.
It is an advantage of the invention that structure novel, the reflecting mirror that script is used to adjust angle between laser pulse is reduced by 6 To 2, by the change of the circle diameter to circular femto-second laser pulse, to adjust the angle between femto-second laser pulse, this Script is needed the time correlation coherent anti-stokes raman scattering technology of 6 femto-second laser pulses adjusting freedom degrees by invention, It is optimized for only adjusting 3 adjusting freedom degrees of circle diameter of 2 reflecting mirrors and circular femto-second laser pulse, substantially increases and be The stability of system, adjustable ease for use and repeatability.
Detailed description of the invention
Fig. 1 is the principle of the present invention figure.
Specific embodiment
Femtosecond pulse generator 1 generate a branch of femtosecond pulse 3, after reflecting mirror 1, beam splitter 6, will Femtosecond pulse 3 is divided into the identical femtosecond pulse 1 of two beam wavelength and femtosecond pulse 25, wherein femtosecond pulse Laser 25 enters optical parametric oscillator 4, and the wavelength for the femtosecond pulse 37 being emitted from optical parametric oscillator 4 can occur Change, realize the adjusting of the wavelength of femtosecond pulse 37 in a certain range, flies by what optical parametric oscillator 4 generated Pulse per second (PPS) laser 37 forms a branch of annulus shape femtosecond pulse 12, the annulus after annulus light generating device 8 Shape femtosecond pulse 12 is closed at dichroscope 11 with the femtosecond pulse 1 after the reflection of reflecting mirror 2 10 Beam, obtains that a branch of coaxial mixing femtosecond pulse, wherein femtosecond pulse 1 is located at circular femtosecond pulse 12 It is intermediate;The coaxial mixing femtosecond pulse converges at the sample among sample cell 14 after convex lens 1, this When the coaxial mixing femtosecond pulse and sample of the centre of sample cell 14 interact, generate a wavelength and converge in The different signal pulse laser 15 of coaxial mixing femtosecond pulse on sample, making the pulse laser through sample includes three kinds Femtosecond pulse 9, annulus shape femtosecond pulse 12 and the signal pulse laser 15 of wavelength, the arteries and veins comprising these three wavelength After reflecting mirror 3 17, optical filter 18, signal pulse laser 15 is retained impulse light, and signal pulse laser 15 is through excess convexity 3 19 shrink beam of lens, is received by photomultiplier tube reception device 20, is recorded and is connected with photomultiplier tube reception device 20 On computer 21.Computer can be recorded under different experimental conditions, by data acquisition software if sample is by femtosecond laser arteries and veins After impulse hair, the information such as intensity and wavelength by the signal pulse laser 15 under the different delays time, and draw corresponding figure Table analyzes experimental result on one side.
11 pairs of the dichroscope circular femtosecond pulses 12 reflect, and carry out to femtosecond pulse 1 saturating It penetrates;
The annulus light generating device 8 is expanded the concavees lens 801, convex lens 802 and annulus of part by femtosecond pulse The 0-2 π spiral phase plate 803 that light generates part forms.
Whole system is placed on uniform optical platform, and femtosecond pulse generator 1 is located at the lower right of whole system, Optical parametric oscillator 4 is located at the left side of femtosecond pulse generator 1, and annulus light generating device 8 is located at optical parametric oscillator The left side of device 4, sample cell 14 are located at femtosecond pulse generator 1, optical parametric oscillator 4 and annulus light generating device 8 Top.

Claims (3)

1. a kind of coaxial femtosecond time Correlated Coherent anti-Stokes Raman scatters test macro, it is characterised in that: femtosecond pulse Laser generator generate a branch of femtosecond pulse, after reflecting mirror one, beam splitter, femtosecond pulse is divided into two beams The identical femtosecond pulse one of wavelength and femtosecond pulse two, wherein femtosecond pulse two enters optical parametric oscillator The wavelength of device, the femtosecond pulse three being emitted from optical parametric oscillator can change, and realize femtosecond pulse three The adjusting of wavelength in a certain range is produced by the femtosecond pulse three that optical parametric oscillator generates using annulus light After generating apparatus, form a branch of annulus shape femtosecond pulse, the annulus shape femtosecond pulse with it is anti-through reflecting mirror two Femtosecond pulse one after penetrating carries out conjunction beam at dichroscope, obtains a branch of coaxial mixing femtosecond pulse, wherein flies Pulse per second (PPS) laser one is located at the centre of circular femtosecond pulse;The coaxial mixing femtosecond pulse passes through convex lens one Afterwards, it converges at the sample among sample cell, at this time the coaxial sample mixed among femtosecond pulse and sample cell It interacts, generating a wavelength, the signal pulse different from the coaxial mixing femtosecond pulse converged on sample swashs Light, making the pulse laser through sample includes femtosecond pulse, annulus shape femtosecond pulse and the signal of three kinds of wavelength Pulse laser, after reflecting mirror three, optical filter, signal pulse laser is retained the pulse laser comprising these three wavelength Come, signal pulse laser passes through three shrink beam of convex lens, is received by photomultiplier tube reception device, is recorded and connects with photomultiplier tube On the computer that receiving apparatus is connected.
2. a kind of coaxial femtosecond time Correlated Coherent anti-Stokes Raman according to claim 1 scatters test macro, It is characterized by: the dichroscope reflects circular femtosecond pulse, femtosecond pulse one is transmitted.
3. a kind of coaxial femtosecond time Correlated Coherent anti-Stokes Raman according to claim 1 scatters test macro, It is characterized by: the annulus light generating device is produced by the concavees lens, convex lens and annulus light that femtosecond pulse expands part The 0-2 π spiral phase plate of first portion forms.
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Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN113155311A (en) * 2021-04-22 2021-07-23 中国工程物理研究院流体物理研究所 CARS temperature measurement method and device
CN114563367A (en) * 2022-03-02 2022-05-31 吉林大学 Circular polarization transient absorption spectrum system for diagnosing coaxial BOXCRS configuration under extreme conditions

Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2002520612A (en) * 1998-07-20 2002-07-09 バッテル・メモリアル・インスティチュート Nonlinear vibration microscopy
CN102116929A (en) * 2011-01-30 2011-07-06 中国科学院西安光学精密机械研究所 High-speed WFOV (wide field of view) CARS (coherent anti-stokes raman scattering) microscope system and method
US20110282166A1 (en) * 2009-12-18 2011-11-17 The Regents Of The University Of California System and Method for Efficient Coherence Anti-Stokes Raman Scattering Endoscopic and Intravascular Imaging and Multimodal Imaging
CN205166175U (en) * 2015-11-17 2016-04-20 北华航天工业学院 Hollow ring beam diameter adjusting device
CN106226284A (en) * 2016-08-23 2016-12-14 深圳大学 Coherent anti-stokes raman scattering spectrographic detection and micro imaging system and method

Patent Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2002520612A (en) * 1998-07-20 2002-07-09 バッテル・メモリアル・インスティチュート Nonlinear vibration microscopy
US20110282166A1 (en) * 2009-12-18 2011-11-17 The Regents Of The University Of California System and Method for Efficient Coherence Anti-Stokes Raman Scattering Endoscopic and Intravascular Imaging and Multimodal Imaging
CN102116929A (en) * 2011-01-30 2011-07-06 中国科学院西安光学精密机械研究所 High-speed WFOV (wide field of view) CARS (coherent anti-stokes raman scattering) microscope system and method
CN205166175U (en) * 2015-11-17 2016-04-20 北华航天工业学院 Hollow ring beam diameter adjusting device
CN106226284A (en) * 2016-08-23 2016-12-14 深圳大学 Coherent anti-stokes raman scattering spectrographic detection and micro imaging system and method

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
朱林泉 等: "《现代激光工程应用技术》", 30 July 2008 *
李志焕: ""螺旋相位板在产生涡旋光束及图像边缘增强中的应用", 《中国优秀硕士学位论文全文数据库 基础科学辑》 *

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN113155311A (en) * 2021-04-22 2021-07-23 中国工程物理研究院流体物理研究所 CARS temperature measurement method and device
CN113155311B (en) * 2021-04-22 2023-04-11 中国工程物理研究院流体物理研究所 CARS temperature measurement method and device
CN114563367A (en) * 2022-03-02 2022-05-31 吉林大学 Circular polarization transient absorption spectrum system for diagnosing coaxial BOXCRS configuration under extreme conditions

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