CN101771237B - Parametric amplification or parametric conversion system of adjustable broadband laser pulse of spectral response curve - Google Patents
Parametric amplification or parametric conversion system of adjustable broadband laser pulse of spectral response curve Download PDFInfo
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- CN101771237B CN101771237B CN2010103003639A CN201010300363A CN101771237B CN 101771237 B CN101771237 B CN 101771237B CN 2010103003639 A CN2010103003639 A CN 2010103003639A CN 201010300363 A CN201010300363 A CN 201010300363A CN 101771237 B CN101771237 B CN 101771237B
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Abstract
The invention relates to a parametric amplification or parametric conversion system of an adjustable broadband laser pulse of a spectral response curve, which belongs to the field of nonlinear intense laser. The parametric amplification or parametric conversion system comprises a spatial frequency chirp transformation device, a splitting, attenuation and optical delay device, a partially reflecting mirror, a focusing cylindrical lens, a fan-shaped periodically poled crystal, a filtering device and a collimating cylindrical lens, wherein the partially reflecting mirror, the focusing cylindrical lens, the fan-shaped periodically poled crystal, the filtering device and the collimating cylindrical lens are arranged on an optical axial line in sequence, the output pump pulse of the splitting, attenuation and optical delay device enters the partially reflecting mirror from a 45-degree angle, and the installation directions of the partially reflecting mirror and the filtering device respectively form a 45-degree included angle with the output optical shaft of the spatial frequency chirp transformation device. The system of the invention not only can realize the parametric amplification or conversion for almost identical gains of all frequency components within the input signal bandwidth, but also can adjust the intensity and the position of each pump pulse according to needs, so as to change the bandwidth or the spectral property of the frequency response curve or the output pulse bandwidth. Moreover, the system has the advantages of simple structure, convenient calibration, flexible crystal selection and the like.
Description
Technical field
The present invention relates to a kind of adjustable broadband laser pulse parameter of input and output spectral response curve of realizing amplifies or converting system; This system can realize that not only the parameter of the gain much at one of all frequency contents in the input signal bandwidth amplifies or conversion; But also can regulate the intensity and the position of each pumping pulse as required; Change the spectral response curve of said parameter amplification or converting system or the bandwidth and the spectral characteristic of output pulse, belong to non-linear light laser field.
Background technology
The parameter of broadband ultrashort laser pulse amplifies (or parameter change) and is different from laser of narrowband, because all there is effect of dispersion inevitably in nonlinear crystal, promptly phase velocity and the group velocity of the light of different frequency in crystal is different.For anisotropic nonlinear crystal, can utilize the birefringence effect of crystal to compensate the phase velocity difference that causes by effect of dispersion, realize phase matching, i.e. birefringent phase matching technique (BPM).Equally, also the birefringence effect of crystal capable of using is realized group velocity coupling (GVM).Yet generally speaking, for the anisotropic nonlinear crystal of major part, these two couplings can't satisfy simultaneously, generally do not overlap because satisfy two matching directions of BPM and GVM.For isotropic nonlinear crystal, can utilize the positive and negative normal chromatic dispersion of crystal to realize what phase matching (PM) and group velocity were mated.Yet these two couplings also can't satisfy simultaneously, because it is normally different to satisfy the ratio of PM and the desired positive and negative normal chromatic dispersion material of GVM.The phase place of at present, amplifying (or parameter change) to broadband parametric mainly comprises with the solution of group velocity matching problem: non-colinear phase matching, wavetilt group velocity coupling, degeneracy point phase matching, multi-angle pumping phase matching and the pumping of time domain delay dipulse are warbled and are mated etc.
These schemes all respectively have relative merits; Non-colinear phase matching and wavetilt group velocity matched optical path are simple in structure, but limited bandwidth, not only light channel structure is simple for degeneracy point phase matching method; And can obtain bigger bandwidth; But crystals with different can only be applied on the specific frequency, though and multi-angle pumping phase matching and time domain postpone the dipulse pumping coupling of warbling and can obtain maximum bandwidth, its complex structure; And multi-angle pumping phase matching is because a plurality of light beams intersect at same position simultaneously, and its power input density is restricted.
Summary of the invention
For improving the bandwidth that the laser pulse parameter amplifies (or parameter change); The object of the invention aims to provide that a kind of simple in structure, adjustment is convenient, crystal selects flexibly that the adjustable broadband laser pulse parameter of spectral response curve amplifies or converting system; The parameter that not only can realize the gain much at one of all frequency contents in the input signal bandwidth amplifies, but also can regulate output bandwidth and response curve as required.
For realizing the foregoing invention purpose; The basic technology scheme that the present invention takes is; The broadband laser pulse parameter that a kind of spectral response curve is adjustable amplifies or the parameter converting system; Comprise spatial frequency warble converting means, beam splitting, decay and optical delay device and be arranged in spatial frequency warble partially reflecting mirror, focusing cylindrical lens, fan-shaped periodic polarized crystal, filter and collimation cylindrical lens on the converting means optical axis successively; The output pumping pulse of wherein beam splitting, decay and optical delay device is 45 ° and is incident to partially reflecting mirror, and the installation direction of said partially reflecting mirror and filter and the spatial frequency converting means output optical axis of warbling is 45 ° of angles.
As specific embodiment; Said pumping pulse beam splitting, decay and deferred mount can be made up of partially reflecting mirror, attenuator, optical delay line and catoptron; The input pumping pulse is incided partially reflecting mirror behind optical delay line, partially reflecting mirror reflected light part is a branch of pumping pulse of output behind adjustable attenuator; Partially reflecting mirror transmitted light part is also exported a branch of pumping pulse after inciding another adjustable attenuator after the mirror reflects.The beam split ratio of partially reflecting mirror can realize through selecting the different piece catoptron.Corresponding increase partially reflecting mirror etc. can obtain more multiple laser pumping pulse, and partially reflecting mirror incides the diverse location of fan-shaped periodic polarized crystal after the pumping laser pulse is divided into 2 bundles or multiple laser light beam by a certain percentage in pumping pulse beam splitting, decay and the deferred mount; Wherein attenuator is used to regulate the intensity of each pumping laser pulse; Optical delay line is used to regulate the time relationship between each pumping laser pulse after time synchronized and the beam splitting of pumping laser pulse and broadband laser pulse.
The said spatial frequency converting means of warbling can be made up of, grating, rib grid, body grating etc. tilt flat plate glass, prism; Broadband laser pulse is transformed into broad-adjustable spatial frequency chirped pulse; And all frequency contents of said spatial frequency chirped pulse are distributed in the diverse location on a certain axle of horizontal space, are parallel to each other.
Said partially reflecting mirror has transmission and reflection function, and the pumping pulse that miter angle is imported reflexes to focusing cylindrical lens, will import broadband laser pulse simultaneously and directly be transmitted to focusing cylindrical lens.
Said focusing cylindrical lens focuses on appropriate location on the fan-shaped periodic polarized crystal axle with each broadband laser pulse of importing.
Said fan-shaped periodic polarized crystal; The variation of polarization cycle on horizontal a certain axle that can satisfy the accurate phase matching of different frequency composition becomes corresponding relation with the change of frequency of spatial frequency chirped pulse; After above-mentioned pulse incident; On spatial frequency is warbled direction, fan-shaped periodic polarized crystal is carried out up-down adjustment, make all frequency contents of spatial frequency chirped pulse can both be in the parallel incident of optimum phase matched position.The spatial frequency chirped pulse both can vertical fan-shaped periodic polarized crystal surface feeding sputtering, also suitably angle tilt incident.
Said filter can adopt dichronic mirror or filter plate, and the different-waveband laser pulse of exporting after the fan-shaped periodic polarized crystal conversion is separated, and exports the laser pulse of required wave band.
Said collimation cylindrical lens is exported behind the laser pulse collimation with dichronic mirror output;
Preferred version according to embodiment is; The said spatial frequency converting means of warbling specifically is made up of the grating lens group that a diffraction grating and convex lens are formed; Wherein the focus of convex lens is in the center of laser pulse incident, and optical axis is consistent to the centre frequency diffraction direction of broadband laser pulse first-order diffraction with diffraction grating.When the broadband of laser pulse was big, said convex lens and focusing cylindrical lens adopted achromat.
Said pumping pulse can the laser of narrowband pulse also can be a broadband laser pulse.In order the different frequency composition to be carried out the regulation and control of space amplitude and phase place; To realize more complicated input and output response curve; Based on above-mentioned basic structure basis, can be in fan-shaped periodic polarized crystal front side or rear side increasing degree spatial light modulator or phase spatial light modulator.
Design concept of the present invention is to utilize pumping laser pulse and wideband pulse different frequency components to realize accurate phase matching (QPM) simultaneously through the diverse location of periodic polarized crystal; Promptly utilize chromatic dispersion elements such as grating or prism to warble converting means with spatially mutual the separating of different frequency components in the wideband pulse as spatial frequency; Become the spatial frequency chirped pulse that the different frequency components light path is parallel to each other; Change pulse incident angle, optical component parameter (like the parameter of grating or prism) and the distance between them; Can be so that the parallel diverse location that incides on the horizontal a certain axle of fan-shaped periodic polarized crystal of different frequency components; With the overlapping and time synchronized in pumping laser pulse implementation space; Realize accurate phase matching (QPM) in different paths, make different frequency components realize that at the diverse location of crystal the parameter of gain much at one amplifies or nonlinear frequency transformation, simultaneously; The also intensity and the position of each pumping pulse light beam of flexible as required change that this parameter amplifies or the bandwidth and the spectral characteristic of the spectral response curve of converting system or output pulse.
The broadband laser pulse parameter that spectral response curve according to the invention is adjustable amplifies or converting system comprises following three major parts:
One is the wideband pulse spatial frequency converting means of warbling; Every can broadband laser pulse be transformed into the device of broad-adjustable spatial frequency chirped pulse can; Usually tilt flat plate glass, prism, grating, rib grid, body grating etc. are made up of, the broadband laser pulse of input is transformed into broad-adjustable spatial frequency chirped pulse through the spatial frequency converting means of warbling;
One is pumping laser pulse beam split, decay and the delay regulating device that is made up of partially reflecting mirror, attenuator and optical delay line, and the pumping laser pulse of input is transformed to 2 bundle or all adjustable laser pulses of multi beam light intensity, position and delay through beam splitting, decay and deferred mount;
One is to be placed on the wideband pulse spatial frequency fan-shaped periodic polarized crystal (or other have the nonlinear optical crystal of similar characteristics) on the output light path of converting means of warbling.Pumping laser pulse and spatial frequency chirped pulse incide fan-shaped periodic polarized crystal synchronously, realize the optimum phase coupling in the different paths of crystal, realize that parameter amplifies or parameter change.
The warble spatial frequency chirped pulse of converting means output of wideband pulse spatial frequency incides on the end face of fan-shaped periodic polarized crystal with the pumping pulse that the delay regulating device is exported with pumping pulse beam split, decay simultaneously; The pumping pulse incoming position can be regulated arbitrarily through the light path of regulating beam split, decay and delay regulating device as required; Make the different frequency composition of different pumping pulse light beams and chirped pulse overlapping at diverse location; And the position of spatial frequency chirped pulse centre frequency also can be regulated; Thereby make the different spectral components of wideband pulse can both realize the optimum phase coupling at diverse location with different pumping laser pulsed light beams; The all spectral components of wideband pulse are interacted with different pumping laser pulsed light beams in different path separately; Realize that broadband parametric is amplified or parameter change efficiently; Regulate the intensity and the position of each pumping pulse light beam, just can change the frequency response curve of parameter amplification or parameter change system or the bandwidth and the spectral characteristic of output pulse easily and flexibly.All incident laser pulses both can impinge perpendicularly in the fan-shaped periodic polarized crystal, angle tilt incident that also can be suitable.Take out required frequency range laser pulse by dichronic mirror after the conversion and by exporting behind the collimation cylindrical lens collimation.
Pumping pulse according to the invention can the laser of narrowband pulse also can be a broadband laser pulse; And on above-mentioned basic structure basis; Can be as required; Increasing degree spatial light modulator, phase spatial light modulator etc. carry out space amplitude and phase place regulation and control to the different frequency composition before and after fan-shaped periodic polarized crystal, to realize more complicated input and output response curve.
Broadband laser pulse parameter according to the invention amplifies or converting system can realize that not only the parameter that all frequency contents gain much at one in the input signal bandwidth amplifies, but also governing response curve or output bandwidth and spectral characteristic as required.Through selecting different periodic polarized crystal parameters for use, this light path system is equally applicable to and optical parameter processes such as frequency, difference frequency, and has characteristics such as simplicity of design, adjustment is convenient, the crystal selection is flexible.
Description of drawings
Fig. 1 is a system schematic of the present invention;
Fig. 2 is that the adjustable broadband laser pulse parameter of spectral response curve amplifies or the converting system synoptic diagram among the embodiment;
Fig. 3 is the three-dimensional structure synoptic diagram of fan-shaped periodic polarized crystal among Fig. 2.
In the accompanying drawings:
The 1-spatial frequency warble converting means 2-beam splitting, the decay with the delay regulating device
The fan-shaped periodic polarized crystal of 3-partially reflecting mirror 4-focusing cylindrical lens 5-
6-filter 7-collimation cylindrical lens 8-diffraction grating 9-convex lens
10-optical delay line 11-catoptron 12-partially reflecting mirror 13-attenuator
Embodiment
Below in conjunction with accompanying drawing and embodiment the present invention is done and to further describe:
Like Fig. 1; Present embodiment provides the adjustable broadband laser pulse parameter of a kind of spectral response curve to amplify or converting system, comprise spatial frequency warble converting means 1 (can by tilt flat plate glass, prism to, rib grid to, body grating to or grating lens group etc. constitute), beam splitting, decay and optical delay device 2 (can form), partially reflecting mirror 3, focusing cylindrical lens 4, fan-shaped periodic polarized crystal 5 (as shown in Figure 3), filter 6 and collimation cylindrical lens 7 by partially reflecting mirror, attenuator and ray delay line etc.The warble spatial frequency chirped pulse of converting means 1 output of wideband pulse spatial frequency incides on the end face of fan-shaped periodic polarized crystal 5 through partially reflecting mirror 3 and focusing cylindrical lens 4 with the pumping pulse that delay regulating device 2 is exported with pumping pulse beam splitting, decay simultaneously; The pumping pulse incoming position can be regulated arbitrarily through the light path of regulating beam split, decay and delay regulating device as required; Make the different frequency composition of different pumping pulse light beams and chirped pulse overlapping at diverse location; And the position of spatial frequency chirped pulse centre frequency also can be regulated; Thereby make the different spectral components of wideband pulse can both realize the optimum phase coupling at diverse location with different pumping laser pulsed light beams; The all spectral components of wideband pulse are interacted with different pumping laser pulsed light beams in different path separately; Realize that broadband parametric is amplified or nonlinear frequency transformation efficiently; Regulate the intensity and the position of each pumping pulse light beam, just can change the frequency response curve of this parameter amplification or converting system or the bandwidth and the spectral characteristic of output pulse easily and flexibly.The laser pulse of all incidents both can impinge perpendicularly in the fan-shaped periodic polarized crystal (among the figure 5), angle tilt incident that also can be suitable.Take out required frequency range laser pulses by dichronic mirror 6 after the conversion and by exporting behind collimation cylindrical lens 7 collimations.
As shown in Figure 2, wherein the spatial frequency grating lens group that converting means 1 is made up of a diffraction grating 8 and convex lens 9 of warbling constitutes.The focus of convex lens 9 is in the center of laser pulse incident, and optical axis is consistent to the centre frequency diffraction direction of laser pulse first-order diffraction with diffraction grating, if achromatic convex lens is more preferably used in the broadband of laser pulse.Broadband laser pulse incides on the diffraction grating 8 with certain angle; Because the dispersion interaction of grating; The angle of diffraction of different frequency composition is different in the pulse, produces the spectrum angular dispersion, through becoming the spatial frequency chirped pulse that each frequency content is parallel to each other and exports behind the convex lens 9; It after partially reflecting mirror 3 and focusing cylindrical lens 4 focus on, incides the diverse location of fan-shaped periodic polarized crystal 5 end faces as the space chirp input pulse.
The fan-shaped periodic polarized crystal 5 of present embodiment is as shown in Figure 3; The polarization cycle of its center path is by the optimum phase matching Design according to the centre frequency of broadband laser pulse and pumping pulse; The fan-out angle of crystal polarization cycle also is to confirm that according to the bandwidth of laser pulse the method for designing of concrete property reference cycle polarized crystal is carried out, because its method for designing is a prior art; Not in the scope of the invention, do not specify at this.The fan-shaped periodic polarized crystal 5 of up-down adjustment on spatial frequency is warbled direction; The frequency content of incident pulse centre frequency is got into from the optimum phase matched position; Realize the harmonic conversion of centre frequency top efficiency, then, the grating constant of change diffraction grating 8 and the incident angle of laser pulse perhaps change the focal length of convex lens 9; The space width of scalable frequency chirp pulse makes other frequency contents also get into fan-shaped periodic polarized crystal 5 with the optimum phase matched position; Pumping pulse is behind optical delay line 10, catoptron 11, partially reflecting mirror 12 and attenuator; Obtain all adjustable 2 bundle pumping pulse light beams of light intensity, position and delay;, partially reflecting mirror 3 and focusing cylindrical lens 4 incide fan-shaped periodic polarized crystal 5 after focusing on equally; Regulate the optical axis position of each pump beam; Make them overlapping with the spectral component of different wideband pulse respectively, all spectral components of wideband pulse are interacted in fan-shaped periodic polarized crystal 5 with different pumping laser pulsed light beams in different path separately, realize that broadband parametric is amplified or nonlinear frequency transformation efficiently; Regulate the intensity and the position of each pumping pulse light beam, just can change the frequency response curve of amplification of this parameter or converting system or the bandwidth and the spectral characteristic of output pulse easily and flexibly.The laser pulse of all incidents both can impinge perpendicularly in the fan-shaped periodic polarized crystal, angle tilt incident that also can be suitable, and concrete angle can be adjusted according to the measurement situation.Take out required frequency range laser pulses by dichronic mirror 6 after the conversion and by exporting behind collimation cylindrical lens 7 collimations.
The foregoing description is not in order to qualification the present invention, any those skilled in the art, and in not breaking away from essence spirit of the present invention and scope, various variations and the modification done should be all in protection scope of the present invention.
Claims (6)
1. the adjustable broadband laser pulse parameter of spectral response curve amplifies or the parameter converting system; It is characterized in that comprising the spatial frequency of importing broadband laser pulse warble beam splitting, decay and the optical delay device (2) of converting means (1), input pumping pulse and warble A partially reflecting mirror (3), focusing cylindrical lens (4), fan-shaped periodic polarized crystal (5), filter (6) and collimation cylindrical lens (7) on converting means (1) optical axis of the spatial frequency of layout successively; The output pumping pulse of wherein beam splitting, decay and optical delay device (2) is 45 ° and is incident to A partially reflecting mirror (3), and the warble output optical axis of converting means (1) of the installation direction of said A partially reflecting mirror (3) and filter (6) and spatial frequency is 45 ° of angles; Said pumping pulse beam splitting, decay and deferred mount (2) are made up of B partially reflecting mirror (12), attenuator (13), optical delay line (10) and catoptron (11); The input pumping pulse is behind optical delay line (10); Be 45 ° and incide B partially reflecting mirror (12); The a branch of pumping pulse of output behind attenuator (13) of the reflected light part of B partially reflecting mirror (12) output; The transmitted light of B partially reflecting mirror (12) output partly is 45 ° and is incident to catoptron (11), and this transmitted light part incides a branch of pumping pulse of another attenuator (13) back output again after catoptron (11) reflection.
2. amplify or the parameter converting system according to the adjustable broadband laser pulse parameter of the said spectral response curve of claim 1; It is characterized in that; The said spatial frequency grating lens group that converting means (1) is made up of a diffraction grating (8) and convex lens (9) of warbling constitutes; Wherein the focus of convex lens (9) is in the center of broadband laser pulse incident, and the optical axis of convex lens (9) is consistent to the centre frequency diffraction direction of broadband laser pulse first-order diffraction with diffraction grating (8).
3. amplify or the parameter converting system according to the adjustable broadband laser pulse parameter of the said spectral response curve of claim 2, it is characterized in that, when the broadband of broadband laser pulse was big, said convex lens (9) and focusing cylindrical lens (4) adopted achromat.
4. amplify or the parameter converting system according to the adjustable broadband laser pulse parameter of the said spectral response curve of one of claim 1-3, it is characterized in that said filter (6) can adopt dichronic mirror or filter plate.
5. amplify or the parameter converting system according to the adjustable broadband laser pulse parameter of the said spectral response curve of one of claim 1-3, it is characterized in that said pumping pulse is laser of narrowband pulse or broadband laser pulse.
6. amplify or the parameter converting system according to the adjustable broadband laser pulse parameter of the said spectral response curve of one of claim 1-3; It is characterized in that, at front side or the rear side increasing degree spatial light modulator or the phase spatial light modulator of fan-shaped periodic polarized crystal (5).
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| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| TWI586467B (en) * | 2012-03-28 | 2017-06-11 | Toray Engineering Company Limited | Laser alignment of the laser beam and the use of laser optical axis alignment method of laser processing device |
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| CN106898937B (en) * | 2017-02-16 | 2019-07-23 | 中国科学院电子学研究所 | Semiconductor laser side face couples the alkali metal laser axially pumped |
| CN107247380B (en) * | 2017-08-11 | 2020-04-03 | 深圳大学 | Double-chirp spectrum optical parametric amplifier and amplification method |
| CN108281877A (en) * | 2018-03-14 | 2018-07-13 | 成都师范学院 | Chirped laser pulse frequency spectrum shaping system based on spectrum angle dispersion |
| CN109659804A (en) * | 2019-01-08 | 2019-04-19 | 中国科学院福建物质结构研究所 | For generating the adjustable broadband orange laser of wave crest |
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Citations (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6359914B1 (en) * | 1999-10-04 | 2002-03-19 | University Of Dayton | Tunable pulsed narrow bandwidth light source |
| CN101592842A (en) * | 2009-07-03 | 2009-12-02 | 湖南大学 | A kind of optical path system for wideband laser pulse high-efficiency harmonic conversion |
-
2010
- 2010-01-15 CN CN2010103003639A patent/CN101771237B/en not_active Expired - Fee Related
Patent Citations (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6359914B1 (en) * | 1999-10-04 | 2002-03-19 | University Of Dayton | Tunable pulsed narrow bandwidth light source |
| CN101592842A (en) * | 2009-07-03 | 2009-12-02 | 湖南大学 | A kind of optical path system for wideband laser pulse high-efficiency harmonic conversion |
Non-Patent Citations (2)
| Title |
|---|
| Karl A.Tillman etc."Femtosecond seeded 150nm-bandwidth optical parametric amplifier for active imaging applications at 1550nm".《Proc.of SPIE》.2005,第5958卷59890R-1-59890R-9. |
| O.V.Chekhlov etc."3J broadband femtosecond optical parametric chirped pulse amplification system".《OPTICS LETTERS》.2006,第31卷(第24期), |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| TWI586467B (en) * | 2012-03-28 | 2017-06-11 | Toray Engineering Company Limited | Laser alignment of the laser beam and the use of laser optical axis alignment method of laser processing device |
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