CN1295559C - Ultrashort chirp pulse photon crystal optical parameter amplifying device - Google Patents
Ultrashort chirp pulse photon crystal optical parameter amplifying device Download PDFInfo
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Abstract
一种超短啁啾脉冲光子晶体光学参量放大装置,其特点是该装置最核心的元件是一三维光子晶体,进入该三维光子晶体的信号光路的光学元件依次是信号光源、第一脉冲发生器、光准直元件、起偏元件、第一展宽器和耦合元件;隔离器和分光元件位于所述的三维光子晶体之后,进入所述的三维光子晶体的另一泵浦光路的光学元件沿泵浦光的前进方向依次是泵浦光激光器、第二脉冲发生器、起偏器、第二展宽器和整形器;隔离器之后是分光元件和压缩器,压缩器之后是信号光接收装置。本发明具有结构简单,容易操作和泵浦效率高的特点。
An ultrashort chirped pulse photonic crystal optical parametric amplifier device is characterized in that the core element of the device is a three-dimensional photonic crystal, and the optical elements of the signal light path entering the three-dimensional photonic crystal are signal light source, first pulse generator, light collimating element, polarizing element, first stretcher and coupling element in sequence; the isolator and the beam splitter are located after the three-dimensional photonic crystal, and the optical elements of another pump light path entering the three-dimensional photonic crystal are pump light laser, second pulse generator, polarizer, second stretcher and shaper in the forward direction of the pump light in sequence; the beam splitter and compressor are after the isolator, and the signal light receiving device is after the compressor. The invention has the characteristics of simple structure, easy operation and high pumping efficiency.
Description
技术领域technical field
本发明是一种超短啁啾脉冲光子晶体光学参量放大装置。主要按照可控制方式发生非线性变化的光学系统来放大超短啁啾脉冲波长信号光。The invention is an ultrashort chirped pulse photonic crystal optical parameter amplification device. The ultra-short chirped pulse wavelength signal light is amplified mainly according to an optical system that changes nonlinearly in a controllable manner.
背景技术Background technique
已有技术中美国普林泽麦斯劳.彼.马克维兹(Przemyslaw.P.Markowicz)等人在“三维光子晶体中强势增加产生三次谐波”(Dramatic Enhancement of Third-harmonic Generation inThree-Dimensional photonic crystals)[Physical Review LettersVol.92,No.8(2004)]一文中论述了关于光在三维光子晶体中产生三次谐波的理论和特性研究,为提供一种放大超短啁啾脉冲光子晶体光学参量放大装置奠定了理论基础。In the prior art, Przemyslaw.P.Markowicz (Przemyslaw.P.Markowicz) and others in the U.S. made a strong increase in three-dimensional photonic crystals to generate third harmonics (Dramatic Enhancement of Third-harmonic Generation in Three-Dimensional photonic crystals)[Physical Review LettersVol.92, No.8(2004)] discusses the theory and characteristics of the third harmonic generated by light in three-dimensional photonic crystals, in order to provide an amplified ultrashort chirped pulse photonic crystal The optical parametric amplification device laid the theoretical foundation.
发明内容Contents of the invention
本发明的目的是提供一种超短啁啾脉冲光子晶体光学参量放大装置,利用信号光经脉冲发生器产生脉冲可调制信号光,将其展宽后在三维光子晶体中传播的非线性效应进行行波放大,再对展宽放大的脉冲进行压缩,实现超短啁啾脉冲信号光的放大。该装置应具有结构简单,容易操作和泵浦效率高的特点。The purpose of the present invention is to provide an ultra-short chirped pulse photonic crystal optical parameter amplification device, which uses the signal light to generate pulse-modulatable signal light through the pulse generator, and performs the nonlinear effect of spreading in the three-dimensional photonic crystal after it is broadened. The wave is amplified, and then the stretched and amplified pulse is compressed to realize the amplification of the ultrashort chirped pulse signal light. The device should have the characteristics of simple structure, easy operation and high pumping efficiency.
本发明的技术解决方案如下:Technical solution of the present invention is as follows:
一种超短啁啾脉冲光子晶体光学参量放大装置,其特点是该装置最核心的元件是一三维光子晶体,进入该三维光子晶体的信号光路的光学元件依次是信号光源、第一脉冲发生器、光准直元件、起偏元件、第一展宽器和耦合元件;隔离器和分光元件位于所述的三维光子晶体之后,进入所述的三维光子晶体的另一泵浦光路的光学元件沿泵浦光的前进方向依次是泵浦光激光器、第二脉冲发生器、起偏器、第二展宽器和整形器;所述的隔离器之后是所述的分光元件和压缩器,压缩器之后是信号光接收装置,而且进入所述三维光子晶体的泵浦光脉冲展宽的脉宽大于信号光脉冲展宽的脉宽,泵浦光脉冲全部包络信号光脉冲。An ultra-short chirped pulse photonic crystal optical parameter amplification device, which is characterized in that the core component of the device is a three-dimensional photonic crystal, and the optical components entering the signal optical path of the three-dimensional photonic crystal are signal light source, first pulse generator in sequence , light collimating element, polarizing element, first stretcher and coupling element; After the isolator and the light splitting element are located at the described three-dimensional photonic crystal, the optical element entering another pump light path of the three-dimensional photonic crystal is along the pump The forward direction of the pump light is the pump light laser, the second pulse generator, the polarizer, the second stretcher and the shaper in turn; after the isolator is the light splitting element and the compressor, and after the compressor is The signal light receiving device, and the pulse width of the pump light pulse entering the three-dimensional photonic crystal is wider than the pulse width of the signal light pulse, and the pump light pulse completely envelopes the signal light pulse.
所述的信号光源是激光器,该激光器和泵浦光激光器为光纤固体激光器,或半导体激光器。The signal light source is a laser, and the laser and the pumping laser are fiber solid-state lasers or semiconductor lasers.
所述的所说的第一脉冲发生器和第二脉冲发生器是电光调制的脉冲发生器。The said first pulse generator and the second pulse generator are electro-optic modulated pulse generators.
所述的起偏元件和起偏器为尼克耳棱镜,或偏振片,或渥拉斯顿棱镜。所述的光准直元件是由半凸球面透镜构成的。The polarizing element and polarizer are Nichols prisms, polarizers, or Wollaston prisms. The light collimating element is composed of a semi-convex spherical lens.
所述的第一展宽器和第二展宽器的结构相同,主要由闪耀光栅、凸面反射镜和凹面反射镜构成,其光路是输入光经闪耀光栅反射、凹面反射镜反射、凸面反射镜反射、再经凹面反射镜反射而输出。The structure of the first stretcher and the second stretcher is the same, mainly composed of a blazed grating, a convex reflector and a concave reflector. Then it is reflected by the concave mirror and output.
所述的耦合元件是微光学透镜构成的。The coupling element is composed of micro-optical lenses.
所述的三维光子晶体是在三维光子晶体衬底上布设若干三维光子晶体点构成的。The three-dimensional photonic crystal is formed by arranging several three-dimensional photonic crystal points on a three-dimensional photonic crystal substrate.
所述的三维光子晶体点是由玻璃内掺杂,或是石英掺杂材料组成,三维光子晶体点的折射率大于三维光子晶体衬底,掺杂的元素是镱、铒稀有元素,所述的三维光子晶体点呈球体形、立方体形、长方体形、菱体形、多面体形或曲线体形;三维光子晶体点之间的排列呈菱形、方形、矩形或多边形。The three-dimensional photonic crystal point is composed of doped glass or quartz doped material, the refractive index of the three-dimensional photonic crystal point is greater than that of the three-dimensional photonic crystal substrate, and the doped elements are rare elements such as ytterbium and erbium. The three-dimensional photonic crystal points are in the shape of a sphere, a cube, a cuboid, a rhombus, a polyhedron or a curve; the arrangement of the three-dimensional photonic crystal points is in the shape of a rhombus, a square, a rectangle or a polygon.
上述的隔离器是磁光隔离器。The above-mentioned isolator is a magneto-optical isolator.
上述的分光元件为平面透射光栅,或透射闪耀光栅,或透射凹面光栅。The above-mentioned light splitting element is a plane transmission grating, or a transmission blazed grating, or a transmission concave grating.
上述的反射元件为平面反射镜,或凹面反射镜。The above-mentioned reflective element is a plane reflector or a concave reflector.
所述的接收装置为CCD二极管列阵探测器,或光电二极管,或光电倍增管,可多通道板,或示波器,或计算机。The receiving device is a CCD diode array detector, or a photodiode, or a photomultiplier tube, or a multi-channel board, or an oscilloscope, or a computer.
所述的整形器为光阑或透镜。The shaper is a diaphragm or a lens.
本发明的超短啁啾脉冲光子晶体光学参量放大装置的优点:The advantages of the ultrashort chirped pulse photonic crystal optical parameter amplification device of the present invention:
1、使用本发明的超短啁啾脉冲光子晶体光学参量放大装置可实现超短脉冲啁啾波长信号光的放大;1. Using the ultrashort chirped pulse photonic crystal optical parameter amplification device of the present invention can realize the amplification of ultrashort pulse chirped wavelength signal light;
2、泵浦的效率高.2. High pump efficiency.
附图说明Description of drawings
图1是本发明超短啁啾脉冲光子晶体光学参量放大装置最佳实施例结构示意图。Fig. 1 is a structural diagram of the best embodiment of the ultrashort chirped pulse photonic crystal optical parametric amplification device of the present invention.
图2是图1中展宽器5的结构示意图。FIG. 2 is a schematic structural diagram of the
图3是图1中A_A剖面结构示意图。Fig. 3 is a schematic diagram of the A_A section structure in Fig. 1 .
图4是图1中B_B剖面结构示意图。Fig. 4 is a schematic diagram of the B_B section structure in Fig. 1 .
图5是图1中压缩器10的结构示意图。FIG. 5 is a schematic structural diagram of the
图6是图1中第二展宽器13的结构示意图。FIG. 6 is a schematic structural diagram of the
图中:1-信号光源 2-第一脉冲发生器 3-光准直元件4-起偏元件 5-第一展宽器 501-闪耀光栅 502-凸面反射镜503-凹面反射镜 6-耦合元件 7-三维光子晶体 701-三维光子晶体衬底 702-三维光子晶体点 8-隔离器 9-分光元件 10-压缩器 1001-凹面闪耀光栅 1002-凹面反射镜11-接收装置 12-整形器 13-第二展宽器 1301-闪耀光栅1302-凸面反射镜 303、凹面反射镜 14-起偏器 15-第二脉冲发生器 16-泵浦光激光器In the figure: 1-signal light source 2-first pulse generator 3-light collimation element 4-polarization element 5-first stretcher 501-blazed grating 502-convex reflector 503-concave reflector 6-coupling element 7 -Three-dimensional photonic crystal 701-Three-dimensional photonic crystal substrate 702-Three-dimensional photonic crystal point 8-Isolator 9-Splitting element 10-Compressor 1001-Concave blazed grating 1002-Concave mirror 11-Receiving device 12-Shaper 13-Part Two stretchers 1301-blazed grating 1302-convex mirror 303, concave mirror 14-polarizer 15-second pulse generator 16-pump laser
具体实施方式:Detailed ways:
先请参阅图1,图1是本发明超短啁啾脉冲光子晶体光学参量放大装置最佳实施例的结构示意图,由图可见,本发明超短啁啾脉冲光子晶体光学参量放大装置,包括,最核心的元件为三维光子晶体7,隔离器8和分光元件9位于三维光子晶体7之后,耦合元件6和展宽器5及起偏元件4置于三维晶体光子7之前,准直光元件3置于起偏元件4之前,置于准直光元件3的入射面之前是脉冲发生器2和信号光源1,置于三维光子晶体7的侧面另一路光学元件是整形器12,展宽器13位于整形器12之前,起偏14位于展宽器13之前,起偏器14之前是脉冲发生器15和泵浦光激光器16,隔离器8之后是分光元件9和压缩器10,压缩器10之后是被放大的信号光接收装置11。First please refer to Fig. 1, Fig. 1 is the structure diagram of the best embodiment of the ultrashort chirped pulse photonic crystal optical parameter amplification device of the present invention, as can be seen from the figure, the ultrashort chirped pulse photonic crystal optical parameter amplification device of the present invention comprises, The core element is the three-dimensional
所说的信号光源1是激光器可为光纤固体激光器,或半导体激光器,泵浦光激光器16是激光二极管,信号光源1发射的光入射到脉冲发生器2上产生脉冲信号光射入准直光元件3,经准直光元件3出射的脉冲信号光被起偏元件4起偏变成线偏振光,该线偏振光入射到展宽器5而被展宽,展宽后的脉冲信号光入射到耦合元件6上,经耦合元件6耦合后的光射入三维光子晶体7内,泵浦光由激光器16出射经脉冲脉冲发生器15产生脉冲泵浦光后进入起偏器14起偏成线偏振光,再经展宽器13展宽后进入整形器12整成所需要的光斑形状后从侧面入射到三维光子晶体7内,泵浦光与信号光在三维光子晶体内耦合被放大之后经隔离器8射入分光元件9,分光元件9将闲置光分离出去后把被放大的信号光送进压缩器10内,压缩器10将信号光压缩成超短脉冲光后入射到信号光的接收装置11上。Said signal light source 1 is a laser, which can be a fiber-optic solid-state laser or a semiconductor laser, and the
所说的构成信号光源1和泵浦光源16是光纤固体激光器,或半导体激光器。The signal light source 1 and the pumping
所说的第一脉冲发生器2和第二脉冲发生器15是电光调制的脉冲发生器。Said
所说的起偏元件4和起偏器14为尼克耳棱镜,或偏振片,或渥拉斯顿棱镜。Said polarizing
所说的准直光元件3是由半凸球面透镜构成的。Said collimating light element 3 is made of semi-convex spherical lens.
所说的展宽器5主要包括闪耀光栅501,凸面反射镜502和凹面反射镜503,如图2所示。The
所说的耦合元件6是由微光学透镜构成的。Said
所说的三维光子晶体7是由玻璃,或是由石英构成的,三维光子晶体横截面如图3和4所示,三维光子晶体衬底701上是三维光子晶体点702,三维光子晶体点702呈球体形,立方体形,长方体形,菱体形,多面体形和曲线体形;702之间的排列呈菱形,方形,矩形和多边形。三维光子晶体点702是由玻璃内掺杂,或是石英掺杂材料组成,三维光子晶体点702多的折射率大于三维光子晶体衬底701,掺杂的元素是镱、铒等稀有元素。Said three-dimensional
所说的分光元件9是平面透射光栅,或是透射闪耀光栅,或是透射凹面光栅构成的。Said light splitting
所说的压缩器10主要包括凹面闪耀光栅1001,凹面反射镜1002,如图5所示。The
所说的接收装置11是CCD二极管列阵探测器,或者是光电二极管,或者是光电倍增管,或者是多通道板,或是示波器,或者是计算机。Said receiving
所说的整形器12是由光阑、透镜构成的。Said
所说的泵浦光路上的第二展宽器13主要包括闪耀光栅1301,凸面反射镜1302和凹面反射镜1303,如图6所示。The
本发明的超短啁啾脉冲光子晶体光学参量放大装置工作过程是:当信号光经脉冲发生器2产生脉冲信号光后经准直光元件3调整成平行光后进入起偏元件4变成平行偏振光,该平行偏振光由第一展宽器5将脉冲展宽,展宽的脉冲存在色散形成啁啾脉冲,展宽了的啁啾脉冲被耦合元件6耦合到三维光子晶体7内,另一路泵浦光由泵浦光激光器发出的光经第二脉冲发生器15产生脉冲泵浦光直入起偏器14后变成线偏振光再经第二展宽器13展宽,泵浦光脉冲展宽的脉宽要大于信号脉冲光的脉宽,在三维光子晶体7内,泵浦光经整形器12整成所需的光斑形状,从三维光子晶体7的侧面进入三维光子晶体7内,泵浦光脉冲要全部包络信号光脉冲,信号光Is与泵浦光Ip在三维光子晶体7内相遇时,由于非线性耦合效应,使信号光Is被放大,由三维光子晶体7放大输出两种光,一种是被放大的信号光Gs,另一种光称为空闲光Gi,两种光经隔离器8和分光元件9之后各波长被分开,隔离器8防止前进的光在遇到光学元件表面时反射回来的光打坏三维光子晶体7,被放大的信号光经压缩器10色散得到补偿,将脉冲信号光压缩成超短的啁啾脉冲,放大后被压缩的信号光输送到接收装置11上。The working process of the ultra-short chirped pulse photonic crystal optical parameter amplification device of the present invention is: when the signal light is generated by the
信号光和泵浦光的耦合放大是利用三维光子晶体中的一种非线性现象,它将一小部分入射光功率转移到频率比其低的斯托克斯波上;其工作原理是基于三维光子晶体的受激拉曼散射(SRS)效应。三维光子晶体中的SRS源于三维光子晶体的三阶非线性效应,表现为泵浦光子、斯托克斯(Stokes)光子与光学支声子之间的相互作用:泵浦光子被介质分子吸收,电子从基态跃迁到虚能级,虚能级的大小是由泵浦光的能量决定的,然后虚能级的电子在信号光的感应下回到振动态的高能级,产生一个与信号光相同频率、相同相位、相同方向的光子,称为斯托克斯光子。如果一个信号光与一个强泵浦光波同时在三维光子晶体内,并且信号光波长位于泵浦光波的拉曼增益谱带宽之内,则此信号光可被该三维光子晶体放大。The coupling amplification of signal light and pump light uses a nonlinear phenomenon in three-dimensional photonic crystals, which transfers a small part of the incident light power to Stokes waves with a lower frequency than it; its working principle is based on three-dimensional photonic Stimulated Raman scattering (SRS) effect of crystals. The SRS in 3D photonic crystals originates from the third-order nonlinear effect of 3D photonic crystals, manifested as the interaction between pump photons, Stokes photons and optical branch phonons: pump photons are absorbed by medium molecules , the electrons transition from the ground state to the virtual energy level, the size of the virtual energy level is determined by the energy of the pump light, and then the electrons in the virtual energy level return to the high energy level of the vibration state under the induction of the signal light, generating a Photons with the same frequency, same phase, and same direction are called Stokes photons. If a signal light and a strong pump light wave are in the three-dimensional photonic crystal at the same time, and the wavelength of the signal light is within the Raman gain spectrum bandwidth of the pump light wave, the signal light can be amplified by the three-dimensional photonic crystal.
在图1所示的装置中,信号光源1是用固体激光器作光源,输出波长是10645nm,输出能量2.7μJ。三维光子晶体点702呈球体形,三维光子晶体衬底是石英,掺杂为铒,信号光为其三倍频354nm。实验表明波长为354nm的信号光被放大600倍以上,脉宽为2.1×10-15秒。In the device shown in Fig. 1, the signal light source 1 uses a solid-state laser as the light source, the output wavelength is 10645 nm, and the output energy is 2.7 μJ. The three-dimensional
经实验表明,本发明装置具有结构简单,容易操作和泵浦效率高的特点。Experiments show that the device of the invention has the characteristics of simple structure, easy operation and high pumping efficiency.
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