CN101706617B - Acousto-optic filter - Google Patents

Acousto-optic filter Download PDF

Info

Publication number
CN101706617B
CN101706617B CN2009102244758A CN200910224475A CN101706617B CN 101706617 B CN101706617 B CN 101706617B CN 2009102244758 A CN2009102244758 A CN 2009102244758A CN 200910224475 A CN200910224475 A CN 200910224475A CN 101706617 B CN101706617 B CN 101706617B
Authority
CN
China
Prior art keywords
lens
acousto
deflector
acoustooptic
lenses
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.)
Active
Application number
CN2009102244758A
Other languages
Chinese (zh)
Other versions
CN101706617A (en
Inventor
李德荣
张春阳
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.)
Changshu intellectual property operation center Co.,Ltd.
Original Assignee
Shenzhen Institute of Advanced Technology of CAS
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 Shenzhen Institute of Advanced Technology of CAS filed Critical Shenzhen Institute of Advanced Technology of CAS
Priority to CN2009102244758A priority Critical patent/CN101706617B/en
Publication of CN101706617A publication Critical patent/CN101706617A/en
Application granted granted Critical
Publication of CN101706617B publication Critical patent/CN101706617B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Landscapes

  • Optical Modulation, Optical Deflection, Nonlinear Optics, Optical Demodulation, Optical Logic Elements (AREA)

Abstract

The invention discloses an acousto-optic filter. The acousto-optic filter comprises two lenses, two acousto-optic deflectors and a liquid crystal spatial light modulator. The focal distances of the two lenses are equal, and the two lenses are arranged in a confocal way; the two acousto-optic deflectors are completely the same and are respectively arranged at the front focal points and the back focal points of the two lenses; and the liquid crystal spatial light modulator is arranged at the common focal point of the lenses and provides an adjustable phase for carrying out color dispersion effect. The invention can realize microsecond stage quick switching between a plurality of wavelength lasers. Furthermore, the collinearity of emergent light beams and incident light beams can be kept, the adjustment of a light path is convenient, and the color dispersion effect of femtosecond lasers is completely eliminated. The invention has compact structure and easy adjustment and can be widely applied to a plurality of research fields of femtosecond laser biologic imaging, optical storage, micro-machining and the like.

Description

Acousto-optic filter
[technical field]
The present invention relates to a kind of acousto-optic filter.
[background technology]
Femtosecond laser has very important application because its duration of pulse is short, the peak power advantages of higher in fields such as bio-imaging, optical storage and microfabrication, is one of focus of domestic and international laser application in recent years.The matter of utmost importance that acousto-optical device is used to control the required solution of femtosecond laser is exactly an effect of dispersion.Effect of dispersion comprises spacial dispersion effect and time dispersive effect.
The acousto-optic crsytal that comprises in the conventional acousto-optical device is a kind of high dispersive medium, and femtosecond laser will be by serious broadening through the acousto-optic crsytal afterpulse, and this effect is called time dispersive (as shown in Figure 1).Simultaneously, have wavelength dependence through the beam deflection angle behind the acousto-optical device (for example acoustooptic deflector), cause the beam divergence distortion, this effect is called spatial dispersion (as shown in Figure 2).These two kinds of effect of dispersions make the advantage of femtosecond laser not exist, and therefore, the matter of utmost importance that acousto-optical device is used to control the required solution of femtosecond laser is exactly an effect of dispersion.
[summary of the invention]
In view of this, be necessary the effect of dispersion problem that exists when being used to control femtosecond laser to provide a kind of acousto-optic filter that can solve the effect of dispersion problem at traditional acousto-optical device.
A kind of acousto-optic filter comprises first lens, second lens, first acoustooptic deflector, second sound light deflector, the LCD space light modulator that are positioned on the same light path; The focal length of first lens and second lens equates, and the back focus of first lens overlaps with the front focus of second lens; First acoustooptic deflector and second sound light deflector are placed on the front focus of first lens and the back focus of second lens respectively, and first acoustooptic deflector and second sound light deflector are identical, and are operated under the identical frequency; LCD space light modulator is placed on the common focus place of first lens and second lens, and the phase place Φ (ω of LCD space light modulator j) satisfy formula I:
Φ ( ω j ) = - 1 2 GDD m ( ω j - ω 0 ) 2 , j ∈ [ - N , N ] - - - ( 1 )
GDD wherein mBe the material dispersion that first acoustooptic deflector and second sound light deflector are introduced, ω 0Be the centre frequency of incident laser, ω jBe the spectral frequency component at j liquid crystal cells place on the LCD space light modulator, N is a natural number.
Preferably, the clear aperature of described first acoustooptic deflector or second sound light deflector is 4.2mm, and crystalline material is TeO 2
Preferably, the design wavelength of described first acoustooptic deflector or second sound light deflector is λ c=800nm, centre frequency is f c=96MHz.
Above-mentioned acousto-optic filter can keep outgoing beam and incident beam conllinear, thereby eliminates the effect of dispersion problem of femtosecond laser fully.And compact conformation is easy to regulate.
[description of drawings]
Fig. 1 is a time dispersive stretched pulse synoptic diagram.
Fig. 2 disperses synoptic diagram for spatial dispersion makes hot spot.
Fig. 3 is the synoptic diagram of acousto-optic filter.
Fig. 4 is the synoptic diagram of acoustooptic deflector transit time.
Fig. 5 is the synoptic diagram of the relation curve of the frequency of operation of first acoustooptic deflector or second sound light deflector and laser wavelength of incidence.
Fig. 6 is the synoptic diagram of each liquid crystal pixel polishing wax frequency distribution of LCD space light modulator.
[embodiment]
The present invention is described in further detail below in conjunction with accompanying drawing and example.
Fig. 3 is the synoptic diagram of acousto-optic filter.Acousto-optic filter comprises first lens 5, second lens 6, first acoustooptic deflector 7, second sound light deflector 8, the LCD space light modulator 9 that is positioned on the same light path.
The focal length (representing with F among the figure) of first lens 5 and second lens 6 equates, and the back focus of first lens 5 overlaps with the front focus of second lens 6.First acoustooptic deflector 7 and second sound light deflector 8 are placed on the front focus of first lens 5 and the back focus of second lens 6 respectively, and first acoustooptic deflector 7 and second sound light deflector 8 are identical, and are operated under the identical frequency.LCD space light modulator 9 is placed on the common focus place of first lens 5 and second lens 6, and the phase place Φ (ω of LCD space light modulator 9 j) satisfied following formula I:
Φ ( ω j ) = - 1 2 GDD m ( ω j - ω 0 ) 2 , j ∈ [ - N , N ] - - - ( I )
GDD wherein mBe the material dispersion that first acoustooptic deflector 7 and second sound light deflector 8 are introduced, ω 0Be the centre frequency of incident laser, ω jBe the spectral frequency component at j liquid crystal cells place on the LCD space light modulator 9, N is a natural number.
Existing commercialization acousto-optical device can be less than the acoustic optic interaction time of 10 microseconds easily, therefore, selects acoustooptic deflector to be used to realize the quick switching of a plurality of wavelength lasers, and its speed can reach the microsecond magnitude fully.
The clear aperature of first acoustooptic deflector 7 or second sound light deflector 8 is 4.2mm, and crystalline material is TeO 2, being operated under unusual Bragg diffraction (Bragg diffraction) pattern, the velocity of propagation of ultrasound wave in crystal is v=650m/s, its maximum transit time is τ Max(the maximum transit time is meant that sound wave passes through the required time of overall optical beam diameter D to=6.5 μ s, and computing formula is τ Max=D/v, as shown in Figure 4).When beam sizes reduced, its transit time can also be littler.Therefore, adopt acoustooptic deflector can realize fully the microsecond level between a plurality of wavelength lasers is switched fast.
When acoustooptic deflector is operated in a certain frequency, after different wavelength of laser enters acoustooptic deflector, will be along different directions outgoing (as shown in Figure 2).The emergent light deflection angle theta that is operated under the unusual Bragg diffraction pattern satisfies formula II:
θ = λf v - - - ( II )
Wherein f is the frequency of operation of acoustooptic deflector, and λ is an optical maser wavelength, and v is hyperacoustic velocity of propagation in the acousto-optic crsytal.
For the ease of using, usually acoustooptic deflector is designed to following situation: when laser wavelength of incidence be the design wavelength of acoustooptic deflector just, and acoustooptic deflector is when being operated in centre frequency, outgoing beam and incident beam maintenance conllinear.In the present invention, the design wavelength of first acoustooptic deflector 7 or second sound light deflector 8 is λ c=800nm, centre frequency is f c=96MHz.Therefore, when laser wavelength of incidence is 800nm, when acoustooptic deflector was operated in 96MHz, outgoing beam and incident beam kept conllinear.
From formula II as can be seen, when laser wavelength of incidence λ changes,, make λ f=λ if change the frequency of operation f of acoustooptic deflector simultaneously cf c, then still can keep beam deflection angle θ constant.Therefore, when the frequency of operation of acoustooptic deflector satisfied formula III, outgoing beam and incident beam can keep conllinear:
f = λ c f c λ - - - ( III )
What Fig. 5 illustrated is the frequency of operation of first acoustooptic deflector 7 or second sound light deflector 8 and the relation curve of laser wavelength of incidence.
Based on above-mentioned principle, when the laser to a plurality of wavelength switches, at first select necessary wavelength, and the frequency of operation of regulating acoustooptic deflector makes it satisfy formula III, thereby make the laser of required wavelength still transmit along former incident direction, the laser of other wavelength then departs from incident direction, can not enter follow-up system.Therefore, this device is actually the acousto-optic filter of a fast tunable.
Femtosecond laser is through behind the acoustooptic deflector, and by formula II as can be known, the spectral component of different wave length will be propagated along different directions, thereby make light beam have certain angle of divergence Δ θ, and this effect is called as spatial dispersion (as shown in Figure 2).The parameter of describing this effect is:
dθ dλ = f v - - - ( IV )
In acousto-optic filter of the present invention (as shown in Figure 3), first acoustooptic deflector 7 passes through the Relay lens inverse imaging of first confocal lens 5 and second lens, 6 compositions on second sound light deflector 8, and two focal lengths of lens equate, do not amplify spatial dispersion.Therefore, femtosecond laser through two acoustooptic deflectors after, the total space dispersion parameters is:
dθ dλ = f 1 - f 2 v - - - ( V )
F wherein 1And f 2Be respectively the frequency of operation of first acoustooptic deflector 7 and second sound light deflector 8.When two acoustooptic deflectors are operated under the same frequency, i.e. f 1=f 2The time, the spatial dispersion of femtosecond laser is eliminated fully.
Femtosecond laser through first acoustooptic deflector 7 and second sound light deflector 8 after, because the velocity of propagation difference of different spectral components in acousto-optic crsytal, have time delay each other, thereby cause pulse strenching, this effect is called as time dispersive (as shown in Figure 1).In the present invention, main time dispersive derives from the acousto-optic crsytal in the acoustooptic deflector.Acousto-optic crsytal material commonly used is TeO 2, be a kind of high dispersive medium, its group delay chromatic dispersion expression formula is:
GDD m = λ 3 2 π c 2 · d 2 n d λ 2 · l - - - ( VI )
Wherein c is the light velocity in the vacuum, and n is the material refractive index, and l is a crystal thickness.
The group delay dispersion measure that single acoustooptic deflector is introduced is about 7000fs 2, the group delay dispersion measure of two acoustooptic deflector introducings is about 14000fs 2, this dispersion measure will be the laser pulse stretching of 100fs to 400fs, and seriously reduces the peak power of femtosecond laser.
Acousto-optic filter of the present invention adopts the time dispersive of 9 pairs of femtosecond lasers of LCD space light modulator to compensate.The elementary cell of LCD space light modulator 9 is liquid crystal pixels, and each pixel is under the effect of extra electric field, and its refractive index will change, thereby to modulating through femto-second laser pulse phase place wherein.In actual applications, can be according to the phase function of the group delay dispersion measure design LCD space light modulator of introducing in the system.
First acoustooptic deflector 7 at the space horizontal spreading, on j liquid crystal pixel, has corresponding spectral component ω with the spectrum of femto-second laser pulse j(as shown in Figure 6).In fact, the group delay chromatic dispersion is the second derivative of spectrum phase about spectral frequency, therefore, for the make-up time chromatic dispersion, only need on LCD space light modulator 9, to add certain phase place, the size of its group delay dispersion measure that provides and the material dispersion equal and opposite in direction of two acoustooptic deflectors are provided, opposite in sign get final product (promptly-GDD m), therefore, added phase function must satisfy formula I on the LCD space light modulator 9.
The number of the liquid crystal pixel on the LCD space light modulator 9 is 2N+1.In actual applications, the liquid crystal cells of LCD space light modulator 9 is meticulous more, and is good more to the compensation effect of time dispersive.
Above-mentioned LCD space light modulator 9 can add phase function arbitrarily by the method for programming, thereby can realize the effect of dispersion amount of size arbitrarily in theory.Based on this principle, can effectively dwindle the bulk of acousto-optic filter of the present invention, make its structure more compact.For example, selecting focal length is the lens of 5cm, and the size of total system can narrow down to about 20cm.In addition, in the process of selecting different wave length, only need the phase function on the corresponding change LCD space light modulator 9, can realize time dispersive effect to the different wave length femtosecond laser, and the structure of modifier again, this will bring great convenience to practical application.
Can see that by above-mentioned analysis the present invention can realize that the microsecond level between a plurality of wavelength lasers switches fast, can keep outgoing beam and incident beam conllinear, is convenient to the adjusting of light path, and eliminates the room and time effect of dispersion of femtosecond laser fully.Its compact conformation is easy to regulate, and can be widely used in numerous research fields such as femtosecond laser bio-imaging, optical storage and microfabrication.
It is to be noted at last, though what the device among the present invention was primarily aimed at is Application of Spectral Laser, but in fact also can be applied to continuous laser fully: because the monochromaticity of continuous laser is better, the influence of spatial dispersion and time dispersive is all less, therefore, not needing to carry out effect of dispersion can normally use.
The above embodiment has only expressed several embodiment of the present invention, and it describes comparatively concrete and detailed, but can not therefore be interpreted as the restriction to claim of the present invention.Should be pointed out that for the person of ordinary skill of the art without departing from the inventive concept of the premise, can also make some distortion and improvement, these all belong to protection scope of the present invention.Therefore, the protection domain of patent of the present invention should be as the criterion with claims.

Claims (3)

1. an acousto-optic filter is characterized in that: comprise first lens, second lens, first acoustooptic deflector, second sound light deflector, the LCD space light modulator that are positioned on the same light path; The focal length of first lens and second lens equates, and the back focus of first lens overlaps with the front focus of second lens; First acoustooptic deflector and second sound light deflector are placed on the front focus of first lens and the back focus of second lens respectively, and first acoustooptic deflector and second sound light deflector are identical, and are operated under the identical frequency; LCD space light modulator is placed on the common focus place of first lens and second lens, and the phase place Φ (ω of LCD space light modulator j) satisfy formula I:
Φ ( ω j ) = - 1 2 GDD m ( ω j - ω 0 ) 2 , j ∈ [ - N , N ] - - - ( I )
GDD wherein mBe the material dispersion that first acoustooptic deflector and second sound light deflector are introduced, ω 0Be the centre frequency of incident laser, ω jBe the spectral frequency component at j liquid crystal cells place on the LCD space light modulator, N is a natural number.
2. acousto-optic filter according to claim 1 is characterized in that: the clear aperature of described first acoustooptic deflector or second sound light deflector is 4.2mm, and crystalline material is TeO 2
3. acousto-optic filter according to claim 1 is characterized in that: the design wavelength of described first acoustooptic deflector or second sound light deflector is λ c=800nm, centre frequency is f c=96MHz.
CN2009102244758A 2009-09-30 2009-11-18 Acousto-optic filter Active CN101706617B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN2009102244758A CN101706617B (en) 2009-09-30 2009-11-18 Acousto-optic filter

Applications Claiming Priority (3)

Application Number Priority Date Filing Date Title
CN200910110741 2009-09-30
CN200910110741.4 2009-09-30
CN2009102244758A CN101706617B (en) 2009-09-30 2009-11-18 Acousto-optic filter

Publications (2)

Publication Number Publication Date
CN101706617A CN101706617A (en) 2010-05-12
CN101706617B true CN101706617B (en) 2011-11-02

Family

ID=42376854

Family Applications (1)

Application Number Title Priority Date Filing Date
CN2009102244758A Active CN101706617B (en) 2009-09-30 2009-11-18 Acousto-optic filter

Country Status (1)

Country Link
CN (1) CN101706617B (en)

Families Citing this family (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101887201B (en) * 2010-06-29 2013-06-05 中国科学院深圳先进技术研究院 Wavelength selecting device
US9535309B2 (en) * 2011-12-28 2017-01-03 Femtonics Kft. Compensator system and method for compensating angular dispersion
CN103592803B (en) * 2013-11-13 2016-08-24 华中科技大学 Multi Colour Lasers bundle dynamic compensation synchronous scanning method based on acousto-optic deflection device
CN105980927B (en) * 2013-12-10 2018-09-18 杜比实验室特许公司 Acousto-optic light beam for optical projection system turns to modulator
EP3740802B1 (en) * 2018-01-15 2023-06-28 Leica Microsystems CMS GmbH Acousto-optical device and method
CN109011194A (en) * 2018-09-13 2018-12-18 邵永红 Visualize photodynamic therapy system
CN113777811B (en) * 2021-08-29 2024-03-29 复旦大学 High-bandwidth composite acousto-optic modulation method based on multiple 4F imaging

Also Published As

Publication number Publication date
CN101706617A (en) 2010-05-12

Similar Documents

Publication Publication Date Title
CN101706617B (en) Acousto-optic filter
CN101738815B (en) Laser three-dimensional scanning device and method
CN101976016B (en) Ultra-short pulse dispersion reshaping and amplitude division technology-based ultrahigh-speed optical imaging system and method
JP5213861B2 (en) Imaging apparatus and method
US20090244415A1 (en) Liquid crystal optical modulation element, liquid crystal optical modulation device and method for driving liquid crystal optical modulation element
Kremer et al. A spatio-temporally compensated acousto-optic scanner for two-photon microscopy providing large field of view.
CN107589613B (en) Multi-soliton synchronous scanning-based multi-point output CARS excitation source device and generation method
CN100504514C (en) Acoustooptic modulator used for femtosecond laser
CN100589010C (en) Novel prism pair pulse chromatic dispersion compensator
CN104641286A (en) Wavelength conversion-type spatial light modulation device
Bechtold et al. Beam shaping and high-speed, cylinder-lens-free beam guiding using acousto-optical deflectors without additional compensation optics
CN203326348U (en) Tunable-wavelength deep ultraviolet light laser
Heberle et al. Electro-optic and acousto-optic laser beam scanners
CN102629066A (en) Laser source device of coherent anti-Stokes Raman scattering microscopic system and production method thereof
CN104076573A (en) Electric control continuous gradual change refractive index electro-optical crystal defector
Metcalf et al. Fully programmable two-dimensional pulse shaper for broadband line-by-line amplitude and phase control
CN103346465A (en) Deep ultraviolet light laser with tunable wavelength
CN101887201B (en) Wavelength selecting device
CN103592803A (en) Multi-color laser beam dynamic compensation synchronous scanning method based on acousto-optic deflector
Xing et al. A 2-GHz discrete-spectrum waveband-division microscopic imaging system
Antonov et al. Switch multiplexer of fiber-optic channels based on multibeam acousto-optic diffraction
Peled et al. Acousto-optics bandwidth broadening in a Bragg cell based on arbitrary synthesized signal methods
CN215452042U (en) Multi-beam, multi-wavelength output laser device
CN108155553A (en) Gain spectral band is switched fast and fine adjustable optical parametric oscillator
CA2912088C (en) Method and system for linearizing non-linear optics

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
C10 Entry into substantive examination
SE01 Entry into force of request for substantive examination
C14 Grant of patent or utility model
GR01 Patent grant
TR01 Transfer of patent right

Effective date of registration: 20200914

Address after: 215500 No.13, Caotang Road, Changshu, Suzhou, Jiangsu Province

Patentee after: Changshu intellectual property operation center Co.,Ltd.

Address before: 1068 No. 518055 Guangdong city in Shenzhen Province, Nanshan District City Xili Road School of Shenzhen University

Patentee before: SHENZHEN INSTITUTES OF ADVANCED TECHNOLOGY

TR01 Transfer of patent right
CI03 Correction of invention patent

Correction item: Patentee|Address

Correct: Shenzhen Advanced Technology Research Institute|518055 1068 Xueyuan Avenue, Shenzhen University Town, Xili, Nanshan District, Shenzhen, Guangdong Province

False: Changshu Intellectual Property Operation Center Co., Ltd.|215500 No. 13, Caodang Road, Changshu City, Suzhou City, Jiangsu Province

Number: 40-02

Volume: 36

CI03 Correction of invention patent