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CN108107641B - Second harmonic generation method and device based on photovoltaic photorefractive diffusion management twin - Google Patents

Second harmonic generation method and device based on photovoltaic photorefractive diffusion management twin Download PDF

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CN108107641B
CN108107641B CN201711435290.2A CN201711435290A CN108107641B CN 108107641 B CN108107641 B CN 108107641B CN 201711435290 A CN201711435290 A CN 201711435290A CN 108107641 B CN108107641 B CN 108107641B
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崔虎
林广�
罗爱平
李洁鹏
徐文成
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    • G02FOPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
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Abstract

一种基于光伏光折变扩散管理孪晶的二次谐波产生方法及装置,该光伏光折变扩散管理孪晶由两块相同材料的光伏光折变晶体沿一个公共晶面镜面对称耦合而成,该方法和装置能够克服存在于单块光伏光折变晶体中的载流子扩散效应所引起的空间孤子光束大角度自偏转以及由孤子光束大角度自偏转所导致的基频光与二次谐波之间的相位失配,还可以保护二次谐波产生过程免受外界环境干扰并防止已产生的二次谐波泄漏到空气中,从而充分地提高二次谐波产生的转换效率。

Figure 201711435290

A second harmonic generation method and device based on photovoltaic photorefractive diffusion management twins. The photovoltaic photorefractive diffusion management twins are formed by symmetrical coupling of two photovoltaic photorefractive crystals of the same material along a common crystal plane. The method and device can overcome the large-angle self-deflection of the spatial soliton beam caused by the carrier diffusion effect existing in a single photovoltaic photorefractive crystal and the large-angle self-deflection of the soliton beam caused by the fundamental frequency light and the two The phase mismatch between subharmonics can also protect the second harmonic generation process from external environment interference and prevent the generated second harmonics from leaking into the air, thereby fully improving the conversion efficiency of second harmonic generation .

Figure 201711435290

Description

基于光伏光折变扩散管理孪晶的二次谐波产生方法及装置Second harmonic generation method and device based on photovoltaic photorefractive diffusion management twin

技术领域technical field

本发明涉及光学二次谐波产生领域,具体涉及一种基于光伏光折变扩散管理孪晶的二次谐波产生方法及装置。The invention relates to the field of optical second harmonic generation, in particular to a second harmonic generation method and device based on photovoltaic photorefractive diffusion management twins.

背景技术Background technique

在光学领域中,二次谐波的产生是一种光学变频效应,已发展成为在相干光源产生中广泛使用的一种激光变频技术,可以用来获得新的激光光源。二次谐波的产生可扩展有限光源的波长范围,以满足工业、农业、国防、医疗和科学研究等各个应用领域对不同波长相干光源的实际需求,因此在扩展激光谱线覆盖范围技术方面,特别是在促进短波段激光技术发展上,发挥着重要的作用。In the field of optics, the generation of the second harmonic is an optical frequency conversion effect, which has been developed into a laser frequency conversion technology widely used in the generation of coherent light sources, and can be used to obtain new laser light sources. The generation of second harmonics can expand the wavelength range of limited light sources to meet the actual needs of coherent light sources with different wavelengths in various application fields such as industry, agriculture, national defense, medical treatment and scientific research. Therefore, in terms of expanding the coverage of laser spectral lines, Especially in promoting the development of short-wavelength laser technology, it plays an important role.

二次谐波的产生是由介质在基频光波电场作用下产生的二阶非线性电极化所引起的一种简并三波混频过程。其中,实现相位匹配是激发二次谐波的必要条件,决定了二次谐波的转换效率和光波质量。目前,业界实现相位匹配的常用方法为双折射相位匹配(Birefringent Phase Matched,简称BPM)和准相位匹配(Quasi-Phase Matched,简称QPM)。其中,双折射相位匹配是利用优良的单轴或双轴非线性晶体的双折射效应和色散特性,通过选择光波的波矢方向和偏振方向来改变基频光与二次谐波折射率的相对大小并使之满足相速度匹配,并通过调整光束在晶体入射面上的入射角来实现双折射相位匹配。然而,当采用该方法来实现相位匹配时,基频光和二次谐波在传输过程中会逐渐分离,从而使转换效率下降,这又称为走离效应。准相位匹配是通过对光学晶体的非线性极化率在一维空间上进行周期性调制来形成极化方向彼此相反的光栅结构,并利用周期为微米量级的光栅提供适当的附加波矢来补偿基频光与二次谐波之间的相位失配,准相位匹配不存在走离效应,可以获得较大的转换效率。但是,由于制作周期极化晶体的工艺非常复杂且难以得到大尺寸的极化晶体,使得利用准相位匹配激发二次谐波的成本较高且较难达到高转换效率。The generation of the second harmonic is a degenerate three-wave mixing process caused by the second-order nonlinear electrical polarization of the medium under the action of the fundamental frequency light wave electric field. Among them, achieving phase matching is a necessary condition for exciting the second harmonic, which determines the conversion efficiency and light wave quality of the second harmonic. At present, the commonly used methods for realizing phase matching in the industry are birefringent phase matching (Birefringent Phase Matched, referred to as BPM) and quasi-phase matching (Quasi-Phase Matched, referred to as QPM). Among them, the birefringence phase matching is to use the birefringence effect and dispersion characteristics of the excellent uniaxial or biaxial nonlinear crystal, and change the relative refractive index of the fundamental frequency light and the second harmonic wave by selecting the wave vector direction and polarization direction of the light wave. The size and make it meet the phase velocity matching, and realize the birefringent phase matching by adjusting the incident angle of the light beam on the incident surface of the crystal. However, when this method is used to achieve phase matching, the fundamental frequency light and the second harmonic will gradually separate during the transmission process, thereby reducing the conversion efficiency, which is also called the walk-off effect. Quasi-phase matching is to form a grating structure with opposite polarization directions by periodically modulating the nonlinear polarizability of the optical crystal in one-dimensional space, and use the period to provide an appropriate additional wave vector for the micron-scale grating to compensate Due to the phase mismatch between the fundamental frequency light and the second harmonic, there is no walk-off effect in quasi-phase matching, and a large conversion efficiency can be obtained. However, due to the complex process of manufacturing periodically polarized crystals and the difficulty of obtaining large-sized polarized crystals, the cost of using quasi-phase matching to excite second harmonics is relatively high and it is difficult to achieve high conversion efficiency.

由于二次谐波的转换效率会随着基频光强度的增加而增加,所以若将基频光经聚焦后射入晶体则可以提高二次谐波的转换效率。但是,当利用双折射相位匹配和准相位匹配在块状的体材料中产生二次谐波时,若经聚焦后的入射光束的宽度较窄,则光束会在衍射效应的作用下很快发散展宽,这将导致基频光和二次谐波的相位很快失配,从而极大地降低二次谐波的转换效率。这个问题可以采用将相互作用的光波限制在波导中传播的方法来解决。光波导是由折射率较低介质包裹折射率较高介质而形成的结构,利用光的全反射原理将光限制在微米量级的区域内传输。光波导包含固化波导和柔性波导两种类型。其中,固化波导是利用离子注入、质子交换和飞秒激光写入等技术在光学晶体、玻璃、半导体和有机聚合物等光学材料中制作出的光波导结构。固化波导的结构是固定的,一旦制成就不能进行更改擦除,这使得固化波导的结构参数不能被调控。而柔性波导是利用光束在光折变材料中诱导出的光感应折射率波导结构。由于通过改变诱导光束的强度轮廓和功率可以调节光感应折射率波导的结构且光感应折射率波导可被重复擦除和写入,因此由光束所诱导出的柔性波导的结构参数可以被灵活调控。Since the conversion efficiency of the second harmonic will increase with the increase of the intensity of the fundamental frequency light, if the fundamental frequency light is focused and injected into the crystal, the conversion efficiency of the second harmonic can be improved. However, when using birefringent phase matching and quasi-phase matching to generate second harmonics in bulk materials, if the width of the focused incident beam is narrow, the beam will quickly diverge under the effect of diffraction Broadening, which will cause the phase mismatch between the fundamental frequency light and the second harmonic, which will greatly reduce the conversion efficiency of the second harmonic. This problem can be solved by confining the interacting light waves to propagate in the waveguide. The optical waveguide is a structure formed by a medium with a lower refractive index wrapped around a medium with a higher refractive index, and uses the principle of total reflection of light to confine light to a micron-scale area for transmission. Optical waveguides include cured waveguides and flexible waveguides. Among them, the solidified waveguide is an optical waveguide structure fabricated in optical materials such as optical crystals, glass, semiconductors, and organic polymers by using technologies such as ion implantation, proton exchange, and femtosecond laser writing. The structure of the cured waveguide is fixed, and once it is manufactured, it cannot be changed and erased, which makes the structural parameters of the cured waveguide unable to be adjusted. The flexible waveguide is a light-induced refractive index waveguide structure induced by light beams in photorefractive materials. Since the structure of the light-sensing refractive index waveguide can be adjusted by changing the intensity profile and power of the induced beam, and the light-sensing refractive index waveguide can be repeatedly erased and written, the structural parameters of the flexible waveguide induced by the light beam can be flexibly adjusted .

在实际应用中,用来诱导出柔性波导的光束要具有不发生衍射展宽的特性,因此用来诱导出柔性波导的光束的最佳选择是采用光折变空间孤子。光折变空间孤子的产生是源于衍射效应引起的展宽被光折变非线性效应引起的约束作用严格补偿的结果。目前已发现了三种稳态光折变空间孤子:屏蔽孤子、光伏孤子和屏蔽光伏孤子;其中,屏蔽孤子存在于有外加电场的非光伏光折变晶体中,光伏孤子存在于无外加电场的光伏光折变晶体中,屏蔽光伏孤子存在于有外加电场的光伏光折变晶体中。一束折射率敏感波长的光在光折变晶体中形成空间孤子的同时便在晶体内部写入了柔性光波导,该波导可以用来引导另一束非折射率敏感波长的光。利用光折变空间孤子诱导出的柔性光波导不仅可以实现用一束弱光引导一束强光,还可以实现二次谐波的高效产生。在实际应用中,亮光折变空间孤子因其具有类似于聚焦光斑的光强分布特性(即光强在孤子中心处最大而在远离孤子中心的地方为零的分布特性)而特别适用于需要强非线性光学效应的二次谐波产生。In practical applications, the light beam used to induce the flexible waveguide should have the characteristics of no diffraction broadening, so the best choice for the light beam used to induce the flexible waveguide is to use photorefractive spatial solitons. The generation of photorefractive spatial solitons is the result of the strict compensation of the broadening caused by the diffraction effect and the constraint effect caused by the nonlinear photorefractive effect. At present, three kinds of steady-state photorefractive solitons have been found: shielding solitons, photovoltaic solitons and shielding photovoltaic solitons; among them, shielding solitons exist in non-photorefractive photorefractive crystals with an external electric field, and photovoltaic solitons exist in non-photorefractive crystals without an external electric field. In photovoltaic photorefractive crystals, shielding photovoltaic solitons exist in photovoltaic photorefractive crystals with an external electric field. A beam of light with a refractive index-sensitive wavelength forms a spatial soliton in the photorefractive crystal, and at the same time a flexible optical waveguide is written inside the crystal, and the waveguide can be used to guide another beam of light with a non-refractive index-sensitive wavelength. The flexible optical waveguide induced by photorefractive spatial solitons can not only guide a beam of strong light with a beam of weak light, but also realize the efficient generation of second harmonics. In practical applications, bright photorefractive spatial solitons are especially suitable for applications that require intense Second harmonic generation of nonlinear optical effects.

在波导中产生二次谐波的优势是波导的约束作用可使光束能量集中,这将容易激发强的非线性效应,从而易于获得高转换效率的二次谐波产生。但是,利用亮光折变空间孤子诱导出柔性波导的方法来产生二次谐波的效果受到光折变晶体内载流子扩散效应的影响。扩散效应会使孤子光束在传输过程中发生横向自偏转(自偏转大小与光束宽度有关,光束越窄则其自偏转越大),导致孤子光束所诱导出的柔性波导是弯曲的。弯曲过大的柔性波导不能有效地同时引导相互作用的基频光和二次谐波,从而不但不能增强二次谐波的转换效率,反而会降低转换效率,甚至导致无法产生二次谐波。因此,要想充分提高柔性波导中产生二次谐波的转换效率,必须有效地抑制扩散效应所引起的孤子光束自偏转。The advantage of generating the second harmonic in the waveguide is that the confinement of the waveguide can concentrate the energy of the beam, which will easily excite strong nonlinear effects, so that it is easy to obtain the second harmonic generation with high conversion efficiency. However, the method of using bright photorefractive space solitons to induce flexible waveguides to generate second harmonics is affected by the carrier diffusion effect in photorefractive crystals. The diffusion effect will cause the soliton beam to undergo lateral self-deflection during transmission (the size of the self-deflection is related to the width of the beam, and the narrower the beam is, the greater the self-deflection will be), resulting in the bending of the flexible waveguide induced by the soliton beam. A flexible waveguide that is too bent cannot effectively guide the interacting fundamental frequency light and the second harmonic at the same time, so that not only the conversion efficiency of the second harmonic cannot be enhanced, but the conversion efficiency will be reduced, and even the second harmonic cannot be generated. Therefore, in order to fully improve the conversion efficiency of the second harmonic generated in the flexible waveguide, the self-deflection of the soliton beam caused by the diffusion effect must be effectively suppressed.

在实践中发现,亮光折变空间孤子在晶体内载流子扩散效应作用下发生自偏转的方向与载流子的类型有关。对于有效载流子为电子的晶体(例如KNSBN晶体),扩散效应使亮光折变空间孤子具有一个与晶体c轴反向的横向加速度并使孤子光束向晶体负c面偏转;而对于有效载流子为空穴的晶体(例如BaTiO3晶体),扩散效应使亮光折变空间孤子具有一个与晶体c轴同向的横向加速度并使孤子光束向晶体正c面偏转。2010年,H.Z.Kang等人利用晶体与空气接触的表面对光束的全反射来抑制扩散效应所引起的光束自偏转,在有外加电场的单块SBN晶体(其有效载流子为电子)中形成了贴着晶体负c面这个自然的直线路径传输的表面亮光折变空间孤子,并利用由表面亮光折变空间孤子所诱导出的晶体表面柔性波导获得了转换效率为83.4%/W的二次谐波产生。It has been found in practice that the direction of self-deflection of bright photorefractive space solitons under the effect of carrier diffusion in the crystal is related to the type of carriers. For crystals in which the effective carriers are electrons (such as KNSBN crystals), the diffusion effect makes the bright photorefractive space solitons have a transverse acceleration opposite to the c-axis of the crystal and deflects the soliton beams to the negative c-plane of the crystal; while for the effective current-carrying For crystals in which the son is a hole (such as BaTiO 3 crystal), the diffusion effect makes the bright photorefractive space soliton have a transverse acceleration in the same direction as the crystal c-axis and deflects the soliton beam to the positive c-plane of the crystal. In 2010, HZKang et al. used the total reflection of the beam on the surface of the crystal in contact with the air to suppress the self-deflection of the beam caused by the diffusion effect, and formed a monolithic SBN crystal (whose effective carriers are electrons) with an external electric field. The surface bright photorefractive space solitons transmitted along the natural straight path of the negative c surface of the crystal, and the second harmonic with a conversion efficiency of 83.4%/W was obtained by using the flexible waveguide on the crystal surface induced by the surface bright photorefractive space solitons waves are generated.

在实践中发现,虽然紧贴晶体表面的晶表柔性波导可以克服扩散效应对二次谐波转换效率的不良影响,但是由于晶表柔性波导与空气的接触面极大,使得在波导中传输的光束易受周围环境的影响(例如环境光的强度、空气的湿度和晶体表面的洁净度),从而使得二次谐波的转换效率很容易被周围环境影响,甚至会导致已产生的二次谐波有部分能量从波导中泄漏到空气中。It is found in practice that although the crystal surface flexible waveguide close to the crystal surface can overcome the adverse effect of the diffusion effect on the second harmonic conversion efficiency, but due to the large contact surface between the crystal surface flexible waveguide and the air, the transmission in the waveguide The light beam is easily affected by the surrounding environment (such as the intensity of ambient light, the humidity of the air, and the cleanliness of the crystal surface), so that the conversion efficiency of the second harmonic is easily affected by the surrounding environment, and even leads to the generated second harmonic Some of the wave's energy leaks out of the waveguide into the air.

发明内容Contents of the invention

本发明实施例公开了一种基于光伏光折变扩散管理孪晶的二次谐波产生方法及装置,能够克服存在于单块光伏光折变晶体中的载流子扩散效应所引起的空间孤子光束大角度自偏转以及由孤子光束大角度自偏转所导致的基频光与二次谐波之间的相位失配,还可以保护二次谐波产生过程免受外界环境干扰并防止已产生的二次谐波泄漏到空气中,从而充分地提高二次谐波产生的转换效率。The embodiment of the present invention discloses a second harmonic generation method and device based on photovoltaic photorefractive diffusion management twins, which can overcome the spatial solitons caused by the carrier diffusion effect existing in a single photovoltaic photorefractive crystal The large-angle self-deflection of the beam and the phase mismatch between the fundamental frequency light and the second harmonic caused by the large-angle self-deflection of the soliton beam can also protect the second harmonic generation process from external environmental interference and prevent the generated The second harmonic leaks into the air, thereby substantially improving the conversion efficiency of the second harmonic generation.

本发明实施例第一方面公开一种基于光伏光折变扩散管理孪晶的二次谐波产生装置,所述光伏光折变扩散管理孪晶由两块相同材料的光伏光折变晶体沿一个公共晶面镜面对称耦合而成,所述装置用于利用亮光伏光折变空间孤子在孪晶内的孪晶面处诱导出以孪晶面为中轴面的晶内条形柔性光波导,以使通过调节基频光和二次谐波在所述波导中的传播常数来实现相位匹配,从而实现二次谐波的高效产生。The first aspect of the embodiments of the present invention discloses a second harmonic generation device based on photovoltaic photorefractive diffusion management twins. The photovoltaic photorefractive diffusion management twins are composed of two photovoltaic photorefractive crystals of the same material along a The common crystal plane is mirror-symmetrically coupled, and the device is used to induce an intracrystalline strip-shaped flexible optical waveguide with the twin plane as the central axis plane at the twin plane in the twin by using bright photovoltaic photorefractive space solitons, Phase matching is achieved by adjusting the propagation constants of the fundamental frequency light and the second harmonic in the waveguide, thereby achieving efficient generation of the second harmonic.

作为一种优选的实施方式,在本发明实施例第一方面中:As a preferred implementation mode, in the first aspect of the embodiment of the present invention:

当所述两块相同材料的光伏光折变晶体的有效载流子均为电子时,所述两块相同材料的光伏光折变晶体的负c面经光学抛光后紧密粘接在一起从而形成电子型的光伏光折变扩散管理孪晶;When the effective carriers of the two photovoltaic photorefractive crystals of the same material are electrons, the negative c-sides of the two photovoltaic photorefractive crystals of the same material are closely bonded together after optical polishing to form Electronic photovoltaic photorefractive diffusion management twinning;

当所述两块相同材料的光伏光折变晶体的有效载流子均为空穴时,所述两块相同材料的光伏光折变晶体的正c面经光学抛光后紧密粘接在一起从而形成空穴型的光伏光折变扩散管理孪晶。When the effective carriers of the two photovoltaic photorefractive crystals of the same material are both holes, the front c-planes of the two photovoltaic photorefractive crystals of the same material are optically polished and tightly bonded together so that Formation of hole-type photovoltaic photorefractive diffusion-managed twins.

作为一种优选的实施方式,在本发明实施例第一方面中:As a preferred implementation mode, in the first aspect of the embodiment of the present invention:

所述电子型的光伏光折变扩散管理孪晶在孪晶面的两边具有相反的载流子扩散效应;The electron-type photovoltaic photorefractive diffusion management twin has opposite carrier diffusion effects on both sides of the twin plane;

所述空穴型的光伏光折变扩散管理孪晶在孪晶面的两边具有相反的载流子扩散效应。The hole-type photovoltaic photorefractive diffusion management twin has opposite carrier diffusion effects on both sides of the twin plane.

作为一种优选的实施方式,在本发明实施例第一方面中,所述二次谐波产生装置还包括精密升降台,所述精密升降台用于放置所述光伏光折变扩散管理孪晶,并使所述光伏光折变扩散管理孪晶的孪晶面平行于水平面,以及用于调节所述光伏光折变扩散管理孪晶的垂直高度。As a preferred implementation, in the first aspect of the embodiment of the present invention, the second harmonic generation device further includes a precision lifting platform, and the precision lifting platform is used to place the photovoltaic photorefractive diffusion management twin , and make the twin planes of the photovoltaic photorefractive diffusion management twins parallel to the horizontal plane, and be used to adjust the vertical height of the photovoltaic photorefractive diffusion management twins.

作为一种优选的实施方式,在本发明实施例第一方面中,所述二次谐波产生装置还包括基频光输入光学器件组、二次谐波输出光学器件组以及背景光双向照明光学器件组,其中:As a preferred implementation, in the first aspect of the embodiment of the present invention, the second harmonic generation device further includes a fundamental frequency light input optical device group, a second harmonic output optical device group, and a background light bidirectional illumination optical device device group, where:

所述基频光输入光学器件组包括基频光源、第一准直凸透镜、第一起偏器和聚焦凸透镜;The fundamental frequency light input optical device group includes a fundamental frequency light source, a first collimating convex lens, a first polarizer and a focusing convex lens;

所述二次谐波输出光学器件组包括第二准直凸透镜和分光镜;The second harmonic output optical device group includes a second collimating convex lens and a beam splitter;

所述背景光双向照明光学器件组包括背景光源、第三准直凸透镜、第二起偏器、半透半反镜、前向照明反射镜、全反镜和背向照明反射镜;The background light two-way illumination optical device group includes a background light source, a third collimating convex lens, a second polarizer, a half mirror, a forward illumination reflector, a total reflection mirror and a back illumination reflector;

所述背景光源,用于提供非相干的背景光;The background light source is used to provide an incoherent background light;

所述第三准直凸透镜,用于将发散的背景光准直为平行光;The third collimating convex lens is used to collimate the divergent background light into parallel light;

所述第二起偏器,用于将准直后的背景光变为偏振方向平行于所述光伏光折变扩散管理孪晶的孪晶面的线偏振光;The second polarizer is used to change the collimated background light into linearly polarized light whose polarization direction is parallel to the twin plane of the photovoltaic photorefractive diffusion management twin;

所述半透半反镜,用于将起偏后的背景光平均分成强度相等的前向照明光和背向照明光;The half-mirror is used to divide the polarized background light into equal-intensity forward illumination light and back illumination light;

所述前向照明反射镜,用于将所述前向照明光反射到所述光伏光折变扩散管理孪晶的前端面;the forward-illuminating reflector for reflecting the forward-illuminating light onto the front face of the photovoltaic photorefractive diffusion management twin;

所述全反镜,用于改变所述背向照明光的方向;The total reflection mirror is used to change the direction of the backlighting light;

所述背向照明反射镜,用于将变向后的背向照明光反射到所述光伏光折变扩散管理孪晶的后端面,以使强度相等的前向照明光和背向照明光在所述光伏光折变扩散管理孪晶内相互平行且对向传输,使得叠加在一起的前向照明光和背向照明光对所述光伏光折变扩散管理孪晶进行双向均匀照射;The back-illumination reflector is used to reflect the reversed back-illumination light to the rear end face of the photovoltaic photorefractive diffusion management twin, so that the forward-illumination light and the back-illumination light with equal intensity The photovoltaic photorefractive diffusion management twins are transmitted in parallel and opposite directions, so that the superimposed forward illumination light and back illumination light perform bidirectional and uniform illumination on the photovoltaic photorefractive diffusion management twins;

所述基频光源,用于提供相干的基频光;The fundamental frequency light source is used to provide coherent fundamental frequency light;

所述第一准直凸透镜,用于将发散的基频光准直为平行光束;The first collimating convex lens is used to collimate the divergent fundamental frequency light into a parallel beam;

所述第一起偏器,用于将准直后的基频光变为偏振方向垂直于所述光伏光折变扩散管理孪晶的孪晶面的线偏振光;The first polarizer is used to change the collimated fundamental frequency light into linearly polarized light whose polarization direction is perpendicular to the twin plane of the photovoltaic photorefractive diffusion management twin;

所述聚焦凸透镜,用于将起偏后的基频光聚焦于所述光伏光折变扩散管理孪晶的前端面上并使聚焦光斑对称分布于孪晶面的两侧;The focusing convex lens is used to focus the polarized fundamental frequency light on the front face of the photovoltaic photorefractive diffusion management twin and distribute the focused light spots symmetrically on both sides of the twin plane;

其中,当背景光源的输出功率被改变时,所述前向照明光和背向照明光的强度亦被改变,从而调节所述光伏光折变扩散管理孪晶内的光伏光折变效应的强度和响应时间;Wherein, when the output power of the background light source is changed, the intensity of the forward illumination light and the back illumination light is also changed, thereby adjusting the intensity of the photovoltaic photorefractive effect in the photovoltaic photorefractive diffusion management twin and response time;

其中,当所述基频光源的输出功率以及所述聚焦凸透镜与所述光伏光折变扩散管理孪晶之间的距离被改变时,所述基频光在所述光伏光折变扩散管理孪晶的前端面上聚焦光斑的光强和尺寸亦被改变,从而调节所述基频光在所述光伏光折变扩散管理孪晶内所受到的光伏光折变非线性自聚焦效应,直至使基频光的自聚焦效应补偿其衍射展宽效应,以使基频光在所述光伏光折变扩散管理孪晶内实现无衍射传输,即基频光在所述光伏光折变扩散管理孪晶内实现亮光伏光折变空间孤子传输,并使基频光光束中心的传输轨迹是一条与所述光伏光折变扩散管理孪晶的孪晶面相重合的直线;Wherein, when the output power of the fundamental frequency light source and the distance between the focusing convex lens and the photovoltaic photorefractive diffusion management twin are changed, the fundamental frequency light will be in the photovoltaic photorefractive diffusion management twin The light intensity and size of the focused light spot on the front face of the crystal are also changed, thereby adjusting the photovoltaic photorefractive nonlinear self-focusing effect that the fundamental frequency light receives in the photovoltaic photorefractive diffusion management twin, until the The self-focusing effect of the fundamental frequency light compensates its diffraction broadening effect, so that the fundamental frequency light can be transmitted without diffraction in the photovoltaic photorefractive diffusion management twin, that is, the fundamental frequency light is transmitted in the photovoltaic photorefractive diffusion management twin Realize the transmission of bright photovoltaic photorefractive spatial solitons, and make the transmission track of the center of the fundamental frequency light beam be a straight line coincident with the twin plane of the photovoltaic photorefractive diffusion management twin;

其中,通过升降所述精密升降台使基频光在所述光伏光折变扩散管理孪晶的前端面上的聚焦光斑中心偏离孪晶面,从而使基频光在方向指向孪晶面的横向加速度作用下的光束中心传输轨迹演变成为一条周期性穿过孪晶面的蛇形曲线;Wherein, by lifting the precision lifting table, the focus spot center of the fundamental frequency light on the front face of the photovoltaic photorefractive diffusion management twin deviates from the twin plane, so that the fundamental frequency light points to the lateral direction of the twin plane The transmission trajectory of the beam center under the action of acceleration evolves into a serpentine curve that periodically passes through the twin plane;

其中,通过升降所述精密升降台来改变基频光在所述光伏光折变扩散管理孪晶的前端面上聚焦光斑的中心位置与孪晶面之间的距离,从而调节基频光在光伏光折变扩散管理孪晶内蛇形传输轨迹的弯曲程度,以使基频光和二次谐波在平行于孪晶面方向上的传播常数满足相位匹配,并达到在二次谐波输出光学器件组的输出端观测到二次谐波;其中,在观测二次谐波时,所述第二准直凸透镜,用于将从所述光伏光折变扩散管理孪晶出射的发散的包含基频光和二次谐波的混合光束准直为平行的混合光束;所述分光镜,用于将所述混合光束中的二次谐波进行反射,以及将所述混合光束中的基频光进行透射,以达到单独观测二次谐波的光强变化;Wherein, the distance between the central position of the focused spot of the fundamental frequency light on the front face of the photovoltaic photorefractive diffusion management twin and the twin plane is changed by lifting the precision lifting table, thereby adjusting the fundamental frequency light on the photovoltaic photorefractive diffusion management twin. Photorefractive diffusion manages the bending degree of the serpentine transmission trajectory in the twin, so that the propagation constants of the fundamental frequency light and the second harmonic in the direction parallel to the twin plane meet the phase matching, and achieve optical The second harmonic is observed at the output end of the device group; wherein, when observing the second harmonic, the second collimating convex lens is used to convert the divergent containing base emitted from the photovoltaic photorefractive diffusion management twin The mixed light beam of frequency light and second harmonic is collimated into a parallel mixed light beam; the beam splitter is used for reflecting the second harmonic in the mixed light beam, and for Transmission is performed to observe the light intensity change of the second harmonic alone;

其中,对所述二次谐波产生装置的运行状态进行调控和优化,以使基频光和二次谐波相干叠加组成的所述混合光束在所述光伏光折变扩散管理孪晶内形成稳定的双色亮光伏光折变空间孤子,并使二次谐波产生达到尽可能大的转换效率。Wherein, the operating state of the second harmonic generation device is regulated and optimized, so that the mixed light beam composed of the fundamental frequency light and the second harmonic coherently superimposed is formed in the photovoltaic photorefractive diffusion management twin Stable two-color bright photovoltaic photorefractive space soliton, and make the second harmonic generation achieve the largest possible conversion efficiency.

本发明实施例第二方面公开一种基于光伏光折变扩散管理孪晶的二次谐波产生方法,所述光伏光折变扩散管理孪晶由两块相同材料的光伏光折变晶体沿一个公共晶面镜面对称耦合而成,所述方法包括:The second aspect of the embodiment of the present invention discloses a second harmonic generation method based on photovoltaic photorefractive diffusion management twins. The photovoltaic photorefractive diffusion management twins are composed of two photovoltaic photorefractive crystals of the same material along a The common crystal surface is mirror-symmetrically coupled, and the method includes:

利用亮光伏光折变空间孤子在孪晶内的孪晶面处诱导出以孪晶面为中轴面的晶内条形柔性光波导,以使通过调节基频光和二次谐波在所述波导中的传播常数来实现相位匹配,从而实现二次谐波的高效产生。Using bright photovoltaic photorefractive spatial solitons to induce an intragranular strip-shaped flexible optical waveguide with the twin plane as the central axis plane at the twin plane in the twin crystal, so that by adjusting the fundamental frequency light and the second harmonic The propagation constant in the waveguide described above is used to achieve phase matching, resulting in efficient generation of the second harmonic.

作为一种优选的实施方式,在本发明实施例第二方面中:当所述两块相同材料的光伏光折变晶体的有效载流子均为电子时,所述两块相同材料的光伏光折变晶体的负c面经光学抛光后紧密粘接在一起从而形成电子型的光伏光折变扩散管理孪晶;当所述两块相同材料的光伏光折变晶体的有效载流子均为空穴时,所述两块相同材料的光伏光折变晶体的正c面经光学抛光后紧密粘接在一起从而形成空穴型的光伏光折变扩散管理孪晶。As a preferred implementation, in the second aspect of the embodiment of the present invention: when the effective carriers of the two photovoltaic photorefractive crystals of the same material are electrons, the photovoltaic photorefractive crystals of the two same materials The negative c-sides of the foldable crystals are optically polished and closely bonded together to form electronic photovoltaic photorefractive diffusion management twins; when the effective carriers of the two photovoltaic photorefractive crystals of the same material are both In the case of holes, the front c-planes of the two photovoltaic photorefractive crystals of the same material are optically polished and closely bonded together to form hole-type photovoltaic photorefractive diffusion management twins.

作为一种优选的实施方式,在本发明实施例第二方面中:所述电子型的光伏光折变扩散管理孪晶在孪晶面的两边具有相反的载流子扩散效应;所述空穴型的光伏光折变扩散管理孪晶在孪晶面的两边具有相反的载流子扩散效应。As a preferred implementation, in the second aspect of the embodiment of the present invention: the electron-type photovoltaic photorefractive diffusion management twin has opposite carrier diffusion effects on both sides of the twin plane; the hole Type photovoltaic photorefractive diffusion-managed twins have opposite carrier diffusion effects on both sides of the twin plane.

作为一种优选的实施方式,在本发明实施例第二方面中,所述方法还包括:As a preferred implementation manner, in the second aspect of the embodiment of the present invention, the method further includes:

将所述光伏光折变扩散管理孪晶放置在精密升降台上,并使所述光伏光折变扩散管理孪晶的孪晶面平行于水平面,以及调节所述光伏光折变扩散管理孪晶的垂直高度。placing the photovoltaic photorefractive diffusion management twins on a precision lifting platform, making the twin planes of the photovoltaic photorefractive diffusion management twins parallel to the horizontal plane, and adjusting the photovoltaic photorefractive diffusion management twins vertical height.

作为一种优选的实施方式,在本发明实施例第二方面中,所述方法还包括:As a preferred implementation manner, in the second aspect of the embodiment of the present invention, the method further includes:

利用背景光源提供非相干的背景光;Use background light sources to provide incoherent background lighting;

通过第三准直凸透镜将发散的背景光准直为平行光;Collimating the divergent background light into parallel light through the third collimating convex lens;

通过第二起偏器将准直后的背景光变为偏振方向平行于所述光伏光折变扩散管理孪晶的孪晶面的线偏振光;changing the collimated background light into linearly polarized light whose polarization direction is parallel to the twin plane of the photovoltaic photorefractive diffusion management twin through the second polarizer;

通过半透半反镜将起偏后的背景光平均分成强度相等的前向照明光和背向照明光;The polarized background light is evenly divided into forward lighting and back lighting with equal intensity through the half mirror;

通过前向照明反射镜将所述前向照明光反射到所述光伏光折变扩散管理孪晶的前端面;reflecting the forward illumination light onto the front face of the photovoltaic photorefractive diffusion management twin via a forward illumination mirror;

利用全反镜改变所述背向照明光的方向;Utilizing a total reflection mirror to change the direction of the backlighting light;

通过背向照明反射镜将变向后的背向照明光反射到所述光伏光折变扩散管理孪晶的后端面,以使强度相等的前向照明光和背向照明光在所述光伏光折变扩散管理孪晶内相互平行且对向传输,使得叠加在一起的前向照明光和背向照明光对所述光伏光折变扩散管理孪晶进行双向均匀照射;The reversed back-illumination light is reflected to the rear end face of the photovoltaic photorefractive diffusion management twin through the back-illumination reflector, so that the forward and back illumination lights with equal intensities The refractive diffusion management twins are parallel to each other and transmitted in opposite directions, so that the superimposed forward illumination light and back illumination light illuminate the photovoltaic photorefractive diffusion management twins bidirectionally and uniformly;

利用基频光源提供相干的基频光;Using a fundamental frequency light source to provide coherent fundamental frequency light;

通过第一准直凸透镜将发散的基频光准直为平行光束;collimating the divergent fundamental frequency light into a parallel beam through the first collimating convex lens;

通过第一起偏器将准直后的基频光变为偏振方向垂直于所述光伏光折变扩散管理孪晶的孪晶面的线偏振光;Transforming the collimated fundamental frequency light into linearly polarized light whose polarization direction is perpendicular to the twin plane of the photovoltaic photorefractive diffusion management twin through the first polarizer;

通过聚焦凸透镜将起偏后的基频光聚焦于所述光伏光折变扩散管理孪晶的前端面上并使聚焦光斑对称分布于孪晶面的两侧;Focusing the polarized fundamental frequency light on the front face of the photovoltaic photorefractive diffusion management twin through a focusing convex lens and making the focused light spots symmetrically distributed on both sides of the twin plane;

通过改变所述背景光源的输出功率来改变所述前向照明光和背向照明光的强度,从而调节所述光伏光折变扩散管理孪晶内的光伏光折变效应的强度和响应时间;changing the intensity of the forward illumination light and the back illumination light by changing the output power of the background light source, thereby adjusting the intensity and response time of the photovoltaic photorefractive effect in the photovoltaic photorefractive diffusion management twin;

通过改变所述基频光源的输出功率以及所述聚焦凸透镜与所述光伏光折变扩散管理孪晶之间的距离来调节基频光在所述光伏光折变扩散管理孪晶的前端面上聚焦光斑的光强和尺寸,从而调节所述基频光在所述光伏光折变扩散管理孪晶内所受到的光伏光折变非线性自聚焦效应,直至使基频光的自聚焦效应补偿其衍射展宽效应,以使基频光在所述光伏光折变扩散管理孪晶内实现无衍射传输,即基频光在所述光伏光折变扩散管理孪晶内实现亮光伏光折变空间孤子传输,并使基频光光束中心的传输轨迹是一条与所述光伏光折变扩散管理孪晶的孪晶面相重合的直线;Adjusting the fundamental frequency light on the front face of the photovoltaic photorefractive diffusion management twin by changing the output power of the fundamental frequency light source and the distance between the focusing convex lens and the photovoltaic photorefractive diffusion management twin focusing the light intensity and size of the light spot, thereby adjusting the photovoltaic photorefractive nonlinear self-focusing effect suffered by the fundamental frequency light in the photovoltaic photorefractive diffusion management twin, until the self-focusing effect of the fundamental frequency light is compensated Its diffraction broadening effect enables the fundamental frequency light to realize non-diffraction transmission in the photovoltaic photorefractive diffusion management twin, that is, the fundamental frequency light realizes bright photovoltaic photorefractive space in the photovoltaic photorefractive diffusion management twin Soliton transmission, and make the transmission track of the center of the fundamental frequency light beam be a straight line coincident with the twin plane of the photovoltaic photorefractive diffusion management twin;

其中,通过升降所述精密升降台使基频光在所述光伏光折变扩散管理孪晶的前端面上的聚焦光斑中心偏离孪晶面,从而使基频光在方向指向孪晶面的横向加速度作用下的光束中心传输轨迹演变成为一条周期性穿过孪晶面的蛇形曲线;Wherein, by lifting the precision lifting table, the focus spot center of the fundamental frequency light on the front face of the photovoltaic photorefractive diffusion management twin deviates from the twin plane, so that the fundamental frequency light points to the lateral direction of the twin plane The transmission trajectory of the beam center under the action of acceleration evolves into a serpentine curve that periodically passes through the twin plane;

其中,通过升降所述精密升降台来改变基频光在所述光伏光折变扩散管理孪晶的前端面上聚焦光斑的中心位置与孪晶面之间的距离,从而调节基频光在光伏光折变扩散管理孪晶内蛇形传输轨迹的弯曲程度,以使基频光和二次谐波在平行于孪晶面方向上的传播常数满足相位匹配,并达到在二次谐波输出光学器件组的输出端观测到二次谐波;其中,在观测二次谐波时,所述第二准直凸透镜,用于将从所述光伏光折变扩散管理孪晶出射的发散的包含基频光和二次谐波的混合光束准直为平行的混合光束;所述分光镜,用于将所述混合光束中的二次谐波进行反射,以及将所述混合光束中的基频光进行透射,以达到单独观测二次谐波的光强变化;Wherein, the distance between the central position of the focused spot of the fundamental frequency light on the front face of the photovoltaic photorefractive diffusion management twin and the twin plane is changed by lifting the precision lifting table, thereby adjusting the fundamental frequency light on the photovoltaic photorefractive diffusion management twin. Photorefractive diffusion manages the bending degree of the serpentine transmission trajectory in the twin, so that the propagation constants of the fundamental frequency light and the second harmonic in the direction parallel to the twin plane meet the phase matching, and achieve optical The second harmonic is observed at the output end of the device group; wherein, when observing the second harmonic, the second collimating convex lens is used to convert the divergent containing base emitted from the photovoltaic photorefractive diffusion management twin The mixed light beam of frequency light and second harmonic is collimated into a parallel mixed light beam; the beam splitter is used for reflecting the second harmonic in the mixed light beam, and for Transmission is performed to observe the light intensity change of the second harmonic alone;

其中,对所述二次谐波产生装置的运行状态进行调控和优化,以使基频光和二次谐波相干叠加组成的所述混合光束在所述光伏光折变扩散管理孪晶内形成稳定的双色亮光伏光折变空间孤子,并使二次谐波产生达到尽可能大的转换效率。Wherein, the operating state of the second harmonic generation device is regulated and optimized, so that the mixed light beam composed of the fundamental frequency light and the second harmonic coherently superimposed is formed in the photovoltaic photorefractive diffusion management twin Stable two-color bright photovoltaic photorefractive space soliton, and make the second harmonic generation achieve the largest possible conversion efficiency.

与现有技术相比,本发明实施例具有以下有益效果:Compared with the prior art, the embodiments of the present invention have the following beneficial effects:

本发明实施例中,通过管理光伏光折变扩散管理孪晶内的载流子扩散效应来抑制具有窄光束宽度的亮光伏光折变空间孤子在载流子扩散效应作用下所发生的大角度自偏转,以使亮光伏光折变空间孤子能够一直在光伏光折变扩散管理孪晶的内部传输而不会偏转到孪晶的表面,从而能够克服存在于单块光伏光折变晶体中的载流子扩散效应所引起的空间孤子光束大角度自偏转以及由孤子光束大角度自偏转所导致的基频光与二次谐波之间的相位失配,还可以保护二次谐波产生过程免受外界环境干扰并防止已产生的二次谐波泄漏到空气中,从而充分地提高二次谐波产生的转换效率。在激光器、全光频率转换器和全光通信等领域中均有很高的实用价值。In the embodiment of the present invention, by managing the diffusion effect of photorefractive photorefractive carriers in twin crystals, the large angle of occurrence of bright photovoltaic photorefractive spatial solitons with narrow beam widths under the effect of carrier diffusion is suppressed. Self-deflection, so that bright photovoltaic photorefractive spatial solitons can always be transported inside the photovoltaic photorefractive diffusion management twins without deflecting to the surface of the twins, thereby being able to overcome the existing in monolithic photovoltaic photorefractive crystals The large-angle self-deflection of the spatial soliton beam caused by the carrier diffusion effect and the phase mismatch between the fundamental frequency light and the second harmonic caused by the large-angle self-deflection of the soliton beam can also protect the second harmonic generation process It is free from external environmental interference and prevents the generated second harmonic from leaking into the air, thereby fully improving the conversion efficiency of the second harmonic generation. It has high practical value in the fields of laser, all-optical frequency converter and all-optical communication.

附图说明Description of drawings

为了更清楚地说明本发明实施例中的技术方案,下面将对实施例中所需要使用的附图作简单地介绍,显而易见地,下面描述中的附图仅仅是本发明的一些实施例,对于本领域普通技术人员来讲,在不付出创造性劳动的前提下,还可以根据这些附图获得其他的附图。In order to more clearly illustrate the technical solutions in the embodiments of the present invention, the following will briefly introduce the accompanying drawings that need to be used in the embodiments. Obviously, the accompanying drawings in the following description are only some embodiments of the present invention. For Those of ordinary skill in the art can also obtain other drawings based on these drawings without making creative efforts.

图1为本发明实施例公开的一种基于光伏光折变扩散管理孪晶的二次谐波产生装置的结构示意图;Figure 1 is a schematic structural diagram of a second harmonic generation device based on photovoltaic photorefractive diffusion management twins disclosed in an embodiment of the present invention;

图2为电子型的光伏光折变扩散管理孪晶的结构示意图;Figure 2 is a schematic diagram of the structure of electronic photovoltaic photorefractive diffusion management twins;

图3为空穴型的光伏光折变扩散管理孪晶的结构示意图;Figure 3 is a schematic diagram of the structure of a hole-type photovoltaic photorefractive diffusion management twin;

图4为本发明实施例公开的亮光伏光折变空间孤子的光束中心在光伏光折变扩散管理孪晶中的传输轨迹示意图;Fig. 4 is a schematic diagram of the transmission track of the beam center of the bright photovoltaic photorefractive spatial soliton disclosed in the embodiment of the present invention in the photovoltaic photorefractive diffusion management twin;

图5为本发明实施例公开的双色亮光伏光折变空间孤子在以孪晶面为中轴面的条形柔性光波导中实现二次谐波相位匹配的原理示意图;Fig. 5 is a schematic diagram of the principle of second harmonic phase matching of the two-color bright photovoltaic photorefractive space soliton disclosed in the embodiment of the present invention in a strip-shaped flexible optical waveguide with the twin plane as the central axis;

其中,1-光伏光折变扩散管理孪晶,1A-光伏光折变晶体,1B-光伏光折变晶体,2-精密升降台,3-基频光源,4-第一准直凸透镜,5-第一起偏器,6-聚焦凸透镜,7-第二准直凸透镜,8-分光镜,9-背景光源,10-第三准直凸透镜,11-第二起偏器,12-半透半反镜,13-前向照明反射镜,14-全反镜,15-背向照明反射镜。Among them, 1-photovoltaic photorefractive diffusion management twins, 1A-photovoltaic photorefractive crystal, 1B-photovoltaic photorefractive crystal, 2-precision lifting platform, 3-fundamental frequency light source, 4-first collimating convex lens, 5 - the first polarizer, 6 - focusing convex lens, 7 - the second collimating convex lens, 8 - beam splitter, 9 - background light source, 10 - the third collimating convex lens, 11 - the second polarizer, 12 - semi-transparent Mirror, 13-forward lighting reflector, 14-full mirror, 15-backward lighting reflector.

具体实施方式Detailed ways

下面将结合本发明实施例中的附图,对本发明实施例中的技术方案进行清楚、完整地描述,显然,所描述的实施例仅是本发明一部分实施例,而不是全部的实施例。基于本发明中的实施例,本领域普通技术人员在没有做出创造性劳动前提下所获得的所有其他实施例,都属于本发明保护的范围。The following will clearly and completely describe the technical solutions in the embodiments of the present invention with reference to the accompanying drawings in the embodiments of the present invention. Obviously, the described embodiments are only some of the embodiments of the present invention, not all of them. Based on the embodiments of the present invention, all other embodiments obtained by persons of ordinary skill in the art without making creative efforts belong to the protection scope of the present invention.

需要说明的是,本发明实施例的术语“包括”和“具有”以及他们的任何变形,意图在于覆盖不排他的包含,例如,包含了一系列步骤或单元的过程、方法、系统、产品或设备不必限于清楚地列出的那些步骤或单元,而是可包括没有清楚地列出的或对于这些过程、方法、产品或设备固有的其它步骤或单元。It should be noted that the terms "comprising" and "having" and any variations thereof in the embodiments of the present invention are intended to cover non-exclusive inclusion, for example, a process, method, system, product or process that includes a series of steps or units. The apparatus is not necessarily limited to those steps or units explicitly listed, but may include other steps or units not explicitly listed or inherent to the process, method, product or apparatus.

本发明实施例公开了一种基于光伏光折变扩散管理孪晶的二次谐波产生方法及装置,该光伏光折变扩散管理孪晶由两块相同材料的光伏光折变晶体沿一个公共晶面镜面对称耦合而成,该方法和装置能够利用亮光伏光折变空间孤子在孪晶内的孪晶面处诱导出以孪晶面为中轴面的晶内条形柔性光波导,使得通过调节基频光和二次谐波在晶内条形柔性光波导中的传播常数来实现相位匹配,从而实现二次谐波的高效产生,能够克服存在于单块光伏光折变晶体中的载流子扩散效应所引起的空间孤子光束大角度自偏转以及由孤子光束大角度自偏转所导致的基频光与二次谐波之间的相位失配,还可以保护二次谐波产生过程免受外界环境干扰并防止已产生的二次谐波泄漏到空气中,从而充分地提高二次谐波产生的转换效率。以下结合附图进行详细描述。The embodiment of the present invention discloses a second harmonic generation method and device based on photovoltaic photorefractive diffusion management twins. The photovoltaic photorefractive diffusion management twins consist of two photovoltaic photorefractive crystals of the same material along a common The method and device can use bright photovoltaic photorefractive space solitons to induce an intracrystalline strip-shaped flexible optical waveguide with the twin plane as the central axis plane at the twin plane in the twin crystal, so that By adjusting the propagation constants of the fundamental frequency light and the second harmonic in the intracrystalline strip-shaped flexible optical waveguide to achieve phase matching, the efficient generation of the second harmonic can be achieved, which can overcome the limitations existing in monolithic photovoltaic photorefractive crystals. The large-angle self-deflection of the spatial soliton beam caused by the carrier diffusion effect and the phase mismatch between the fundamental frequency light and the second harmonic caused by the large-angle self-deflection of the soliton beam can also protect the second harmonic generation process It is free from external environmental interference and prevents the generated second harmonic from leaking into the air, thereby fully improving the conversion efficiency of the second harmonic generation. A detailed description is given below in conjunction with the accompanying drawings.

请参阅图1,图1为本发明实施例公开的一种基于光伏光折变扩散管理孪晶的二次谐波产生装置的结构示意图。如图1所示,该基于光伏光折变扩散管理孪晶的二次谐波产生装置可以包括:Please refer to FIG. 1 . FIG. 1 is a schematic structural diagram of a second harmonic generation device based on photovoltaic photorefractive diffusion management twins disclosed in an embodiment of the present invention. As shown in Figure 1, the second harmonic generation device based on photovoltaic photorefractive diffusion management twins may include:

光伏光折变扩散管理孪晶1,其中,光伏光折变扩散管理孪晶1由相同材料的光伏光折变晶体1A和光伏光折变晶体1B沿一个公共晶面镜面对称耦合而成;The photovoltaic photorefractive diffusion management twin 1, wherein the photovoltaic photorefractive diffusion management twin 1 is formed by symmetrically coupling a photovoltaic photorefractive crystal 1A and a photovoltaic photorefractive crystal 1B along a common crystal plane;

精密升降台2,用于放置光伏光折变扩散管理孪晶1,并使光伏光折变扩散管理孪晶1的孪晶面平行于水平面,以及用于调节光伏光折变扩散管理孪晶1的垂直高度;The precision lifting platform 2 is used to place the photovoltaic photorefractive diffusion management twin 1, and make the twin plane of the photovoltaic photorefractive diffusion management twin 1 parallel to the horizontal plane, and to adjust the photovoltaic photorefractive diffusion management twin 1 the vertical height of

如图1所示,该基于光伏光折变扩散管理孪晶的二次谐波产生装置还包括基频光输入光学器件组、二次谐波输出光学器件组以及背景光双向照明光学器件组,其中:As shown in Figure 1, the second harmonic generation device based on photovoltaic photorefractive diffusion management twins also includes a fundamental frequency light input optical device group, a second harmonic output optical device group, and a background light bidirectional illumination optical device group, in:

基频光输入光学器件组包括基频光源3、第一准直凸透镜4、第一起偏器5和聚焦凸透镜6;The fundamental frequency light input optical device group includes a fundamental frequency light source 3, a first collimating convex lens 4, a first polarizer 5 and a focusing convex lens 6;

二次谐波输出光学器件组包括第二准直凸透镜7和分光镜8;The second harmonic output optical device group includes a second collimating convex lens 7 and a beam splitter 8;

背景光双向照明光学器件组包括背景光源9、第三准直凸透镜10、第二起偏器11、半透半反镜12、前向照明反射镜13、全反镜14和背向照明反射镜15。The background light two-way illumination optical device group includes a background light source 9, a third collimating convex lens 10, a second polarizer 11, a half-transparent mirror 12, a forward illumination reflector 13, a total reflection mirror 14 and a back illumination reflector 15.

其中,光伏光折变扩散管理孪晶1是实现二次谐波产生的核心部件,其由相同材料的光伏光折变晶体1A和光伏光折变晶体1B沿一个公共晶面(即孪晶面)镜面对称耦合而成。如图2所示,当光伏光折变晶体1A和光伏光折变晶体1B的有效载流子均为电子时,可以将光伏光折变晶体1A和光伏光折变晶体1B的负c面经光学抛光后紧密粘接在一起从而形成电子型的光伏光折变扩散管理孪晶;或者,如图3所示,当光伏光折变晶体1A和光伏光折变晶体1B的有效载流子均为空穴时,可以将光伏光折变晶体1A和光伏光折变晶体1B的正c面经光学抛光后紧密粘接在一起从而形成空穴型的光伏光折变扩散管理孪晶。需要指出的是,上述电子型的光伏光折变扩散管理孪晶在孪晶面的两边具有相反的载流子扩散效应;同样,上述空穴型的光伏光折变扩散管理孪晶在孪晶面的两边也具有相反的载流子扩散效应。Among them, the photovoltaic photorefractive diffusion management twin 1 is the core component to realize the second harmonic generation. ) are mirror-symmetrically coupled. As shown in Figure 2, when the effective carriers of the photovoltaic photorefractive crystal 1A and the photovoltaic photorefractive crystal 1B are electrons, the negative c-planes of the photovoltaic photorefractive crystal 1A and the photovoltaic photorefractive crystal 1B can be passed through After optical polishing, they are tightly bonded together to form electronic photovoltaic photorefractive diffusion management twins; or, as shown in Figure 3, when the effective carriers of photovoltaic photorefractive crystal 1A and photovoltaic photorefractive crystal 1B are both When it is a hole, the positive c-sides of the photovoltaic photorefractive crystal 1A and the photovoltaic photorefractive crystal 1B can be closely bonded together after optical polishing to form a hole-type photovoltaic photorefractive diffusion management twin. It should be pointed out that the electron-type photovoltaic photorefractive diffusion management twins have opposite carrier diffusion effects on both sides of the twin plane; similarly, the hole-type photovoltaic photorefractive diffusion management twins The two sides of the face also have opposite carrier diffusion effects.

在图1所示的基于光伏光折变扩散管理孪晶的二次谐波产生装置中:In the second harmonic generation device based on photovoltaic photorefractive diffusion management twins shown in Figure 1:

背景光源9,用于提供非相干的背景光;Background light source 9, for providing incoherent background light;

第三准直凸透镜10,用于将发散的背景光准直为平行光;The third collimating convex lens 10 is used to collimate the divergent background light into parallel light;

第二起偏器11,用于将准直后的背景光变为偏振方向平行于光伏光折变扩散管理孪晶1的孪晶面(即平行于Y轴)的线偏振光;The second polarizer 11 is used to change the collimated background light into linearly polarized light whose polarization direction is parallel to the twin plane of the photovoltaic photorefractive diffusion management twin 1 (that is, parallel to the Y axis);

半透半反镜12,用于将起偏后的背景光平均分成强度相等的前向照明光和背向照明光;Half mirror 12, used to divide the polarized background light into forward lighting light and back lighting light with equal intensity;

前向照明反射镜13,用于将前向照明光反射到光伏光折变扩散管理孪晶1的前端面;A forward lighting reflector 13, used to reflect the forward lighting light to the front face of the photovoltaic photorefractive diffusion management twin 1;

全反镜14,用于改变背向照明光的方向;Total mirror 14, used to change the direction of backlighting light;

背向照明反射镜15,用于将变向后的背向照明光反射到光伏光折变扩散管理孪晶1的后端面,以使强度相等的前向照明光和背向照明光在光伏光折变扩散管理孪晶1内相互平行且对向传输,使得叠加在一起的前向照明光和背向照明光对光伏光折变扩散管理孪晶1进行双向均匀照射;The back-illumination reflector 15 is used to reflect the reversed back-illumination light to the rear end face of the photovoltaic photorefractive diffusion management twin 1, so that the forward-illumination light and the back-illumination light with equal intensity are in the same direction as the photovoltaic light. The refractive diffusion management twins 1 are parallel to each other and transmitted in opposite directions, so that the superimposed forward illumination light and back illumination light illuminate the photovoltaic photorefractive diffusion management twins 1 bidirectionally and uniformly;

基频光源3,用于提供相干的基频光;The fundamental frequency light source 3 is used to provide coherent fundamental frequency light;

第一准直凸透镜4,用于将发散的基频光准直为平行光束;The first collimating convex lens 4 is used to collimate the divergent fundamental frequency light into a parallel beam;

第一起偏器5,用于将准直后的基频光变为偏振方向垂直于光伏光折变扩散管理孪晶1的孪晶面(即平行于X轴)的线偏振光;The first polarizer 5 is used to change the collimated fundamental frequency light into linearly polarized light whose polarization direction is perpendicular to the twin plane of the photovoltaic photorefractive diffusion management twin 1 (that is, parallel to the X axis);

聚焦凸透镜6,用于将起偏后的基频光聚焦于光伏光折变扩散管理孪晶1的前端面上并使聚焦光斑对称分布于孪晶面的两侧;The focusing convex lens 6 is used to focus the polarized fundamental frequency light on the front face of the photovoltaic photorefractive diffusion management twin 1 and distribute the focused light spots symmetrically on both sides of the twin plane;

其中,当背景光源9的输出功率被改变时,前向照明光和背向照明光的强度亦被改变,从而调节光伏光折变扩散管理孪晶1内的光伏光折变效应的强度和响应时间;Wherein, when the output power of the background light source 9 is changed, the intensity of the forward illumination light and the back illumination light is also changed, thereby adjusting the intensity and response of the photovoltaic photorefractive effect in the photovoltaic photorefractive diffusion management twin 1 time;

其中,当基频光源3的输出功率以及聚焦凸透镜6与光伏光折变扩散管理孪晶1之间的距离被改变时,基频光在光伏光折变扩散管理孪晶1的前端面上聚焦光斑的光强和尺寸亦被改变,从而调节基频光在光伏光折变扩散管理孪晶1内所受到的光伏光折变非线性自聚焦效应,直至使基频光的自聚焦效应补偿其衍射展宽效应,以使基频光在光伏光折变扩散管理孪晶1内实现无衍射传输,即基频光在光伏光折变扩散管理孪晶1内实现亮光伏光折变空间孤子传输,并使基频光光束中心的传输轨迹是一条与光伏光折变扩散管理孪晶1的孪晶面相重合的直线;Wherein, when the output power of the fundamental frequency light source 3 and the distance between the focusing convex lens 6 and the photovoltaic photorefractive diffusion management twin 1 are changed, the fundamental frequency light is focused on the front face of the photovoltaic photorefractive diffusion management twin 1 The light intensity and size of the light spot are also changed, thereby adjusting the photovoltaic photorefractive nonlinear self-focusing effect suffered by the fundamental frequency light in the photovoltaic photorefractive diffusion management twin 1, until the self-focusing effect of the fundamental frequency light compensates for its Diffraction broadening effect, so that the fundamental frequency light can be transmitted without diffraction in the photovoltaic photorefractive diffusion management twin 1, that is, the fundamental frequency light can realize bright photovoltaic photorefractive spatial soliton transmission in the photovoltaic photorefractive diffusion management twin 1, And make the transmission track of the center of the fundamental frequency light beam be a straight line coincident with the twin plane of the photovoltaic photorefractive diffusion management twin 1;

其中,通过升降精密升降台2使基频光在光伏光折变扩散管理孪晶1的前端面上的聚焦光斑中心偏离孪晶面,从而使基频光在方向指向孪晶面的横向加速度作用下的光束中心传输轨迹演变成为一条周期性穿过孪晶面的蛇形曲线;如图4所示,(a)和(b)分别描述了基频光光束中心从光伏光折变扩散管理孪晶1的光伏光折变晶体1A和光伏光折变晶体1B入射时的传输轨迹;Among them, by lifting the precision lifting table 2, the center of the focused spot of the fundamental frequency light on the front face of the photovoltaic photorefractive diffusion management twin 1 deviates from the twin plane, so that the fundamental frequency light points to the lateral acceleration of the twin plane The transmission trajectory of the beam center below evolves into a serpentine curve that periodically passes through the twin plane; Transmission track of photovoltaic photorefractive crystal 1A and photovoltaic photorefractive crystal 1B incident on crystal 1;

其中,通过升降精密升降台2来改变基频光在光伏光折变扩散管理孪晶1的前端面上聚焦光斑的中心位置与孪晶面之间的距离,从而调节基频光在光伏光折变扩散管理孪晶1内蛇形传输轨迹的弯曲程度(参见图4,图4中的实线、点线和虚线分别为基频光光束中心从光伏光折变扩散管理孪晶1的前端面上三个不同位置入射时的传输情况),以使基频光和二次谐波在平行于孪晶面方向上的传播常数满足相位匹配,并达到在二次谐波输出光学器件组的输出端观测到二次谐波;其中,在观测二次谐波时,第二准直凸透镜7,用于将从光伏光折变扩散管理孪晶1出射的发散的包含基频光和二次谐波的混合光束准直为平行的混合光束;分光镜8,用于将混合光束中的二次谐波进行反射,以及将混合光束中的基频光进行透射,以达到单独观测二次谐波的光强变化;Among them, the distance between the central position of the focused light spot of the fundamental frequency light on the front face of the photovoltaic photorefractive diffusion management twin 1 and the twin plane is changed by lifting the precision lifting platform 2, thereby adjusting the fundamental frequency light on the photovoltaic photorefractive diffusion management twin. The bending degree of the serpentine transmission track in the variable diffusion management twin 1 (see Fig. 4, the solid line, dotted line and dashed line in Fig. The transmission conditions when incident at three different positions above), so that the propagation constants of the fundamental frequency light and the second harmonic in the direction parallel to the twin plane meet the phase matching, and reach the output of the second harmonic output optical device group The second harmonic is observed at the end; wherein, when observing the second harmonic, the second collimating convex lens 7 is used to divert the emitted light from the photovoltaic photorefractive diffusion management twin 1 including the fundamental frequency light and the second harmonic The mixed light beam of the wave is collimated into a parallel mixed light beam; the beam splitter 8 is used to reflect the second harmonic in the mixed light beam, and transmit the fundamental frequency light in the mixed light beam to achieve separate observation of the second harmonic light intensity changes;

其中,对二次谐波产生装置的运行状态进行调控和优化,以使基频光和二次谐波相干叠加组成的所述混合光束在光伏光折变扩散管理孪晶1内形成稳定的双色亮光伏光折变空间孤子,并使二次谐波产生达到尽可能大的转换效率。Wherein, the operating state of the second harmonic generation device is regulated and optimized, so that the mixed light beam composed of the fundamental frequency light and the second harmonic coherently superimposed forms a stable two-color light in the photovoltaic photorefractive diffusion management twin 1 Bright photovoltaic photorefractive space solitons and enables second harmonic generation to achieve the largest possible conversion efficiency.

此外,基于图1所描述的基于光伏光折变扩散管理孪晶的二次谐波产生装置,本发明实施例还公开了一种基于光伏光折变扩散管理孪晶的二次谐波产生方法。在该方法中,光伏光折变扩散管理孪晶1由相同材料的光伏光折变晶体1A和光伏光折变晶体1B沿一个公共晶面镜面对称耦合而成。该方法可以利用亮光伏光折变空间孤子在孪晶内的孪晶面处诱导出以孪晶面为中轴面的晶内条形柔性光波导,以使通过调节基频光和二次谐波在所述波导中的传播常数来实现相位匹配,从而实现二次谐波的高效产生。在该方法中,当光伏光折变晶体1A和光伏光折变晶体1B的有效载流子均为电子时,可以将光伏光折变晶体1A和光伏光折变晶体1B的负c面经光学抛光后紧密粘接在一起从而形成电子型的光伏光折变扩散管理孪晶;或者,当光伏光折变晶体1A和光伏光折变晶体1B的有效载流子均为空穴时,可以将光伏光折变晶体1A和光伏光折变晶体1B的正c面经光学抛光后紧密粘接在一起从而形成空穴型的光伏光折变扩散管理孪晶。上述电子型的光伏光折变扩散管理孪晶在孪晶面的两边具有相反的载流子扩散效应;同样,上述空穴型的光伏光折变扩散管理孪晶在孪晶面的两边也具有相反的载流子扩散效应。该方法主要包括以下步骤:In addition, based on the second harmonic generation device based on photovoltaic photorefractive diffusion management twins described in Figure 1, the embodiment of the present invention also discloses a second harmonic generation method based on photovoltaic photorefractive diffusion management twins . In this method, the photovoltaic photorefractive diffusion management twin 1 is formed by symmetrically coupling a photovoltaic photorefractive crystal 1A and a photovoltaic photorefractive crystal 1B along a common crystal plane. This method can use bright photovoltaic photorefractive spatial solitons to induce an intracrystalline strip-shaped flexible optical waveguide with the twin plane as the central axis plane at the twin plane in the twin crystal, so that by adjusting the fundamental frequency light and the second harmonic The propagation constant of the wave in the waveguide is used to achieve phase matching, resulting in efficient generation of the second harmonic. In this method, when the effective carriers of the photovoltaic photorefractive crystal 1A and the photovoltaic photorefractive crystal 1B are both electrons, the negative c-planes of the photovoltaic photorefractive crystal 1A and the photovoltaic photorefractive crystal 1B can be optically After polishing, they are tightly bonded together to form electronic photovoltaic photorefractive diffusion management twins; or, when the effective carriers of photovoltaic photorefractive crystal 1A and photovoltaic photorefractive crystal 1B are both holes, the The positive c-planes of the photovoltaic photorefractive crystal 1A and the photovoltaic photorefractive crystal 1B are closely bonded together after optical polishing to form hole-type photovoltaic photorefractive diffusion management twins. The above-mentioned electron-type photovoltaic photorefractive diffusion management twins have opposite carrier diffusion effects on both sides of the twin plane; similarly, the above-mentioned hole-type photovoltaic photorefractive diffusion management twins also have opposite carrier diffusion effects on both sides of the twin plane. The opposite carrier diffusion effect. The method mainly includes the following steps:

步骤1:将光伏光折变扩散管理孪晶1放置在精密升降台2上,并使光伏光折变扩散管理孪晶1的孪晶面平行于水平面,以及调节光伏光折变扩散管理孪晶1的垂直高度;Step 1: Place the photovoltaic photorefractive diffusion management twin 1 on the precision lifting platform 2, and make the twin plane of the photovoltaic photorefractive diffusion management twin 1 parallel to the horizontal plane, and adjust the photovoltaic photorefractive diffusion management twin a vertical height of 1;

步骤2:利用背景光源9提供非相干的背景光;通过第三准直凸透镜10将发散的背景光准直为平行光;通过第二起偏器11将准直后的背景光变为偏振方向平行于光伏光折变扩散管理孪晶1的孪晶面(即平行于Y轴)的线偏振光;通过半透半反镜12将起偏后的背景光平均分成强度相等的前向照明光和背向照明光;通过前向照明反射镜13将前向照明光反射到光伏光折变扩散管理孪晶的前端面;利用全反镜14改变背向照明光的方向;通过背向照明反射镜15将变向后的背向照明光反射到光伏光折变扩散管理孪晶1的后端面,以使强度相等的前向照明光和背向照明光在光伏光折变扩散管理孪晶1内相互平行且对向传输,使得叠加在一起的前向照明光和背向照明光对光伏光折变扩散管理孪晶1进行双向均匀照射;Step 2: Utilize the background light source 9 to provide incoherent background light; use the third collimating convex lens 10 to collimate the divergent background light into parallel light; pass the second polarizer 11 to change the collimated background light into a polarization direction Linearly polarized light parallel to the twin plane of photovoltaic photorefractive diffusion management twin 1 (that is, parallel to the Y axis); through the half mirror 12, the polarized background light is equally divided into forward illumination light with equal intensity and backlighting light; the forward lighting light is reflected to the front face of the photovoltaic photorefractive diffusion management twin by the forward lighting reflector 13; the direction of the backlighting light is changed by the full reflection mirror 14; The mirror 15 reflects the reversed back illumination light to the rear end face of the photovoltaic photorefractive diffusion management twin 1, so that the forward illumination light and the back illumination light with equal intensity can pass through the photovoltaic photorefractive diffusion management twin 1. The interiors are parallel to each other and transmitted in opposite directions, so that the superimposed forward illumination light and back illumination light can uniformly irradiate the photovoltaic photorefractive diffusion management twin 1 in two directions;

步骤3:利用基频光源3提供相干的基频光;通过第一准直凸透镜4将发散的基频光准直为平行光束;通过第一起偏器5将准直后的基频光变为偏振方向垂直于光伏光折变扩散管理孪晶1的孪晶面(即平行于X轴)的线偏振光;通过聚焦凸透镜6将起偏后的基频光聚焦于光伏光折变扩散管理孪晶1的前端面上并使聚焦光斑对称分布于孪晶面的两侧;Step 3: Utilize the fundamental frequency light source 3 to provide coherent fundamental frequency light; through the first collimating convex lens 4, the divergent fundamental frequency light is collimated into a parallel beam; through the first polarizer 5, the collimated fundamental frequency light becomes Linearly polarized light whose polarization direction is perpendicular to the twin plane of the photovoltaic photorefractive diffusion management twin 1 (that is, parallel to the X axis); through the focusing convex lens 6, the polarized fundamental frequency light is focused on the photovoltaic photorefractive diffusion management twin The front face of the crystal 1 and the focused spot are symmetrically distributed on both sides of the twin plane;

步骤4:通过改变背景光源9的输出功率来改变前向照明光和背向照明光的强度,从而调节光伏光折变扩散管理孪晶1内的光伏光折变效应的强度和响应时间;Step 4: Change the intensity of the forward illumination light and the back illumination light by changing the output power of the background light source 9, thereby adjusting the intensity and response time of the photovoltaic photorefractive effect in the photovoltaic photorefractive diffusion management twin 1;

步骤5:通过改变基频光源3的输出功率以及聚焦凸透镜6与光伏光折变扩散管理孪晶1之间的距离来调节基频光在光伏光折变扩散管理孪晶1的前端面上聚焦光斑的光强和尺寸,从而调节基频光在光伏光折变扩散管理孪晶1内所受到的光伏光折变非线性自聚焦效应,直至使基频光的自聚焦效应补偿其衍射展宽效应,以使基频光在光伏光折变扩散管理孪晶1内实现无衍射传输,即基频光在光伏光折变扩散管理孪晶1内实现亮光伏光折变空间孤子传输,并使基频光光束中心的传输轨迹是一条与光伏光折变扩散管理孪晶1的孪晶面相重合的直线;Step 5: Adjust the focus of the fundamental frequency light on the front face of the photovoltaic photorefractive diffusion management twin 1 by changing the output power of the fundamental frequency light source 3 and the distance between the focusing convex lens 6 and the photovoltaic photorefractive diffusion management twin 1 The light intensity and size of the light spot, so as to adjust the photovoltaic photorefractive nonlinear self-focusing effect of the fundamental frequency light in the photovoltaic photorefractive diffusion management twin 1, until the self-focusing effect of the fundamental frequency light compensates for its diffraction broadening effect , so that the fundamental frequency light can be transmitted without diffraction in the photovoltaic photorefractive diffusion management twin 1, that is, the fundamental frequency light can realize bright photovoltaic photorefractive spatial soliton transmission in the photovoltaic photorefractive diffusion management twin 1, and make the fundamental The transmission track of the frequency light beam center is a straight line coincident with the twin plane of the photovoltaic photorefractive diffusion management twin 1;

步骤6:通过升降精密升降台2使基频光在光伏光折变扩散管理孪晶1的前端面上的聚焦光斑中心偏离孪晶面,从而使基频光在方向指向孪晶面的横向加速度作用下的光束中心传输轨迹演变成为一条周期性穿过孪晶面的蛇形曲线;Step 6: Make the focus spot center of the fundamental frequency light on the front face of the photovoltaic photorefractive diffusion management twin 1 deviate from the twin plane by lifting the precision lifting platform 2, so that the fundamental frequency light points to the lateral acceleration of the twin plane in the direction The transmission track of the beam center under the action evolves into a serpentine curve that periodically passes through the twin plane;

步骤7:通过升降精密升降台2来改变基频光在光伏光折变扩散管理孪晶1的前端面上聚焦光斑的中心位置与孪晶面之间的距离,从而调节基频光在光伏光折变扩散管理孪晶1内蛇形传输轨迹的弯曲程度,以使基频光和二次谐波在平行于孪晶面方向上的传播常数满足相位匹配,并达到在二次谐波输出光学器件组的输出端观测到二次谐波;其中,在观测二次谐波时,通过第二准直凸透镜7将从光伏光折变扩散管理孪晶1出射的发散的包含基频光和二次谐波的混合光束准直为平行的混合光束;然后,再通过分光镜8将混合光束中的二次谐波进行反射,以及将混合光束中的基频光进行透射,以达到单独观测二次谐波的光强变化;Step 7: Change the distance between the central position of the focused light spot of the fundamental frequency light on the front face of the photovoltaic photorefractive diffusion management twin 1 and the twin plane by lifting the precision lifting platform 2, thereby adjusting the distance between the fundamental frequency light and the photovoltaic light Refractive diffusion manages the bending degree of the serpentine transmission trajectory in twin 1, so that the propagation constants of the fundamental frequency light and the second harmonic in the direction parallel to the twin plane meet the phase matching, and achieve the second harmonic output optical The output end of the device group observes the second harmonic; wherein, when observing the second harmonic, the divergent light emitted from the photovoltaic photorefractive diffusion management twin 1 includes the fundamental frequency light and the second harmonic through the second collimating convex lens 7 The mixed light beam of the subharmonic is collimated into a parallel mixed light beam; then, the second harmonic in the mixed light beam is reflected by the beam splitter 8, and the fundamental frequency light in the mixed light beam is transmitted to achieve separate observation of the two Light intensity variation of sub-harmonic;

步骤8:重复步骤4到步骤7,对二次谐波产生装置的运行状态进行调控和优化,以使基频光和二次谐波相干叠加组成的混合光束在光伏光折变扩散管理孪晶1内形成稳定的双色亮光伏光折变空间孤子,并使二次谐波产生达到尽可能大的转换效率。Step 8: Repeat steps 4 to 7 to adjust and optimize the operating state of the second harmonic generation device, so that the mixed beam composed of the fundamental frequency light and the second harmonic coherently superimposed on the photovoltaic photorefractive diffusion management twin 1 to form a stable two-color bright photovoltaic photorefractive space soliton, and make the second harmonic generation achieve the largest possible conversion efficiency.

本发明实施例中,产生二次谐波的物理机制如下:当亮光伏光折变空间孤子在光伏光折变扩散管理孪晶1内围绕和紧贴着孪晶面做蛇形曲线传输的同时就诱导出了一个以孪晶面为中轴面的条形光感应折射率柔性光波导,该波导反过来约束和引导基频光和二次谐波在该波导中传输和相互作用;在该波导中产生二次谐波的相位匹配条件是只需要使基频光和二次谐波在平行于孪晶面方向上的传播常数满足β=2βω(如图5所示),而并不需要使基频光和二次谐波的波矢满足k=2kω。当调节亮光伏光折变空间孤子在光伏光折变扩散管理孪晶1中的蛇形传输轨迹的弯曲程度时,就同时调节了由亮光伏光折变空间孤子所诱导的条形光感应折射率柔性光波导的弯曲程度,也就相应地调节了基频光和二次谐波在条形光感应折射率柔性光波导中的传播常数在平行于孪晶面方向上的分量;当条形光感应折射率柔性光波导的弯曲程度恰当时,基频光和二次谐波在平行于孪晶面方向上的传播常数就会满足相位匹配。In the embodiment of the present invention, the physical mechanism for generating the second harmonic is as follows: when the bright photovoltaic photorefractive spatial solitons are transmitted in a serpentine curve around and close to the twin planes in the photovoltaic photorefractive diffusion management twin 1 A strip-shaped light-induced refractive index flexible optical waveguide with the twin plane as the central axis plane is induced, which in turn constrains and guides the fundamental frequency light and the second harmonic to transmit and interact in the waveguide; in this The phase matching condition for generating the second harmonic in the waveguide is only to make the propagation constants of the fundamental frequency light and the second harmonic in the direction parallel to the twin plane satisfy β = 2β ω (as shown in Figure 5), and It is not necessary for the wave vectors of the fundamental frequency light and the second harmonic to satisfy k =2k ω . When adjusting the bending degree of the serpentine transmission track of the bright photovoltaic photorefractive space soliton in the photovoltaic photorefractive diffusion management twin 1, the stripe light-induced refraction induced by the bright photovoltaic photorefractive space soliton is simultaneously adjusted The bending degree of the flexible optical waveguide of the index is adjusted accordingly, and the components of the propagation constants of the fundamental frequency light and the second harmonic in the strip-shaped light-induced refractive index flexible optical waveguide in the direction parallel to the twin plane are adjusted accordingly; when the strip-shaped When the bending degree of the light-sensitive refractive index flexible optical waveguide is appropriate, the propagation constants of the fundamental frequency light and the second harmonic in the direction parallel to the twin plane will meet the phase matching.

在图5中,(a)和(b)分别为基频光光束中心从光伏光折变扩散管理孪晶1的光伏光折变晶体1A和光伏光折变晶体1B入射时的相位匹配原理示意图。其中,kω和k分别为基频光和二次谐波的波矢,βω和β分别为基频光和二次谐波在平行于孪晶面方向上的传播常数。In Figure 5, (a) and (b) are schematic diagrams of the phase matching principle when the center of the fundamental frequency light beam is incident from the photovoltaic photorefractive crystal 1A and photovoltaic photorefractive crystal 1B of the photovoltaic photorefractive diffusion management twin 1 . Among them, k ω and k are the wave vectors of the fundamental frequency light and the second harmonic wave, respectively, and β ω and β are the propagation constants of the fundamental frequency light and the second harmonic wave in the direction parallel to the twin plane, respectively.

本发明实施例公开的基于光伏光折变扩散管理孪晶的二次谐波产生方法及装置可以通过管理光伏光折变扩散管理孪晶内的载流子扩散效应来抑制具有窄光束宽度的亮光伏光折变空间孤子在载流子扩散效应作用下所发生的大角度自偏转,以使亮光伏光折变空间孤子能够一直在光伏光折变扩散管理孪晶的内部传输而不会偏转到孪晶的表面,从而能够克服存在于单块光伏光折变晶体中的载流子扩散效应所引起的空间孤子光束大角度自偏转以及由孤子光束大角度自偏转所导致的基频光与二次谐波之间的相位失配,还可以保护二次谐波产生过程免受外界环境干扰并防止已产生的二次谐波泄漏到空气中,从而充分地提高二次谐波产生的转换效率。在激光器、全光频率转换器和全光通信等领域中均有很高的实用价值。The second harmonic generation method and device based on photovoltaic photorefractive diffusion management twins disclosed in the embodiments of the present invention can suppress bright beams with narrow beam widths by managing the carrier diffusion effect in photovoltaic photorefractive diffusion management twins. The large-angle self-deflection of photovoltaic photorefractive space solitons under the action of carrier diffusion effect, so that bright photovoltaic photorefractive space solitons can always be transported inside the photovoltaic photorefractive diffusion management twins without deflecting to The surface of the twin crystal can overcome the large-angle self-deflection of the spatial soliton beam caused by the carrier diffusion effect existing in the monolithic photovoltaic photorefractive crystal and the fundamental frequency light and the two The phase mismatch between the sub-harmonics can also protect the second harmonic generation process from external environmental interference and prevent the generated second harmonics from leaking into the air, thereby fully improving the conversion efficiency of the second harmonic generation . It has high practical value in the fields of laser, all-optical frequency converter and all-optical communication.

以上对本发明实施例公开的一种基于光伏光折变扩散管理孪晶的二次谐波产生方法及装置进行了详细介绍,本文中应用了具体个例对本发明的原理及实施方式进行了阐述,以上实施例的说明只是用于帮助理解本发明的方法及其核心思想;同时,对于本领域的一般技术人员,依据本发明的思想,在具体实施方式及应用范围上均会有改变之处,综上所述,本说明书内容不应理解为对本发明的限制。The method and device for generating second harmonics based on photovoltaic photorefractive diffusion management twins disclosed in the embodiments of the present invention are described above in detail. In this paper, specific examples are used to illustrate the principle and implementation of the present invention. The description of the above embodiments is only used to help understand the method of the present invention and its core idea; meanwhile, for those of ordinary skill in the art, according to the idea of the present invention, there will be changes in the specific implementation and scope of application. In summary, the contents of this specification should not be construed as limiting the present invention.

Claims (6)

1.一种基于光伏光折变扩散管理孪晶的二次谐波产生装置,其特征在于,所述光伏光折变扩散管理孪晶由两块相同材料的光伏光折变晶体沿一个公共晶面镜面对称耦合而成,所述装置用于利用亮光伏光折变空间孤子在孪晶内的孪晶面处诱导出以孪晶面为中轴面的晶内条形柔性光波导,以使通过调节基频光和二次谐波在所述波导中的传播常数来实现相位匹配,从而实现二次谐波的高效产生;1. A second harmonic generation device based on photovoltaic photorefractive diffusion management twins, characterized in that, the photovoltaic photorefractive diffusion management twins are composed of two photovoltaic photorefractive crystals of the same material along a common crystal Surface-mirror surface symmetric coupling, the device is used to induce an intracrystalline strip-shaped flexible optical waveguide with the twin plane as the central axis plane at the twin plane in the twin by using bright photovoltaic photorefractive space solitons, so that Phase matching is achieved by adjusting the propagation constants of the fundamental frequency light and the second harmonic in said waveguide, thereby achieving efficient generation of the second harmonic; 所述二次谐波产生装置还包括精密升降台,所述精密升降台用于放置所述光伏光折变扩散管理孪晶,并使所述光伏光折变扩散管理孪晶的孪晶面平行于水平面,以及用于调节所述光伏光折变扩散管理孪晶的垂直高度;The second harmonic generation device also includes a precision lifting platform, the precision lifting platform is used to place the photovoltaic photorefractive diffusion management twins, and make the twin planes of the photovoltaic photorefractive diffusion management twins parallel in the horizontal plane, and for adjusting the vertical height of the photovoltaic photorefractive diffusion management twins; 所述二次谐波产生装置还包括基频光输入光学器件组、二次谐波输出光学器件组以及背景光双向照明光学器件组,其中:The second harmonic generation device also includes a fundamental frequency light input optical device group, a second harmonic output optical device group, and a background light bidirectional illumination optical device group, wherein: 所述基频光输入光学器件组包括基频光源、第一准直凸透镜、第一起偏器和聚焦凸透镜;The fundamental frequency light input optical device group includes a fundamental frequency light source, a first collimating convex lens, a first polarizer and a focusing convex lens; 所述二次谐波输出光学器件组包括第二准直凸透镜和分光镜;The second harmonic output optical device group includes a second collimating convex lens and a beam splitter; 所述背景光双向照明光学器件组包括背景光源、第三准直凸透镜、第二起偏器、半透半反镜、前向照明反射镜、全反镜和背向照明反射镜;The background light two-way illumination optical device group includes a background light source, a third collimating convex lens, a second polarizer, a half mirror, a forward illumination reflector, a total reflection mirror and a back illumination reflector; 所述背景光源,用于提供非相干的背景光;The background light source is used to provide an incoherent background light; 所述第三准直凸透镜,用于将发散的背景光准直为平行光;The third collimating convex lens is used to collimate the divergent background light into parallel light; 所述第二起偏器,用于将准直后的背景光变为偏振方向平行于所述光伏光折变扩散管理孪晶的孪晶面的线偏振光;The second polarizer is used to change the collimated background light into linearly polarized light whose polarization direction is parallel to the twin plane of the photovoltaic photorefractive diffusion management twin; 所述半透半反镜,用于将起偏后的背景光平均分成强度相等的前向照明光和背向照明光;The half-mirror is used to divide the polarized background light into equal-intensity forward illumination light and back illumination light; 所述前向照明反射镜,用于将所述前向照明光反射到所述光伏光折变扩散管理孪晶的前端面;the forward-illuminating reflector for reflecting the forward-illuminating light onto the front face of the photovoltaic photorefractive diffusion management twin; 所述全反镜,用于改变所述背向照明光的方向;The total reflection mirror is used to change the direction of the backlighting light; 所述背向照明反射镜,用于将变向后的背向照明光反射到所述光伏光折变扩散管理孪晶的后端面,以使强度相等的前向照明光和背向照明光在所述光伏光折变扩散管理孪晶内相互平行且对向传输,使得叠加在一起的前向照明光和背向照明光对所述光伏光折变扩散管理孪晶进行双向均匀照射;The back-illumination reflector is used to reflect the reversed back-illumination light to the rear end face of the photovoltaic photorefractive diffusion management twin, so that the forward-illumination light and the back-illumination light with equal intensity The photovoltaic photorefractive diffusion management twins are transmitted in parallel and opposite directions, so that the superimposed forward illumination light and back illumination light perform bidirectional and uniform illumination on the photovoltaic photorefractive diffusion management twins; 所述基频光源,用于提供相干的基频光;The fundamental frequency light source is used to provide coherent fundamental frequency light; 所述第一准直凸透镜,用于将发散的基频光准直为平行光束;The first collimating convex lens is used to collimate the divergent fundamental frequency light into a parallel beam; 所述第一起偏器,用于将准直后的基频光变为偏振方向垂直于所述光伏光折变扩散管理孪晶的孪晶面的线偏振光;The first polarizer is used to change the collimated fundamental frequency light into linearly polarized light whose polarization direction is perpendicular to the twin plane of the photovoltaic photorefractive diffusion management twin; 所述聚焦凸透镜,用于将起偏后的基频光聚焦于所述光伏光折变扩散管理孪晶的前端面上并使聚焦光斑对称分布于孪晶面的两侧;The focusing convex lens is used to focus the polarized fundamental frequency light on the front face of the photovoltaic photorefractive diffusion management twin and distribute the focused light spots symmetrically on both sides of the twin plane; 其中,当背景光源的输出功率被改变时,所述前向照明光和背向照明光的强度亦被改变,从而调节所述光伏光折变扩散管理孪晶内的光伏光折变效应的强度和响应时间;Wherein, when the output power of the background light source is changed, the intensity of the forward illumination light and the back illumination light is also changed, thereby adjusting the intensity of the photovoltaic photorefractive effect in the photovoltaic photorefractive diffusion management twin and response time; 其中,当所述基频光源的输出功率以及所述聚焦凸透镜与所述光伏光折变扩散管理孪晶之间的距离被改变时,所述基频光在所述光伏光折变扩散管理孪晶的前端面上聚焦光斑的光强和尺寸亦被改变,从而调节所述基频光在所述光伏光折变扩散管理孪晶内所受到的光伏光折变非线性自聚焦效应,直至使基频光的自聚焦效应补偿其衍射展宽效应,以使基频光在所述光伏光折变扩散管理孪晶内实现无衍射传输,即基频光在所述光伏光折变扩散管理孪晶内实现亮光伏光折变空间孤子传输,并使基频光光束中心的传输轨迹是一条与所述光伏光折变扩散管理孪晶的孪晶面相重合的直线;Wherein, when the output power of the fundamental frequency light source and the distance between the focusing convex lens and the photovoltaic photorefractive diffusion management twin are changed, the fundamental frequency light will be in the photovoltaic photorefractive diffusion management twin The light intensity and size of the focused light spot on the front face of the crystal are also changed, thereby adjusting the photovoltaic photorefractive nonlinear self-focusing effect that the fundamental frequency light receives in the photovoltaic photorefractive diffusion management twin, until the The self-focusing effect of the fundamental frequency light compensates its diffraction broadening effect, so that the fundamental frequency light can be transmitted without diffraction in the photovoltaic photorefractive diffusion management twin, that is, the fundamental frequency light is transmitted in the photovoltaic photorefractive diffusion management twin Realize the transmission of bright photovoltaic photorefractive spatial solitons, and make the transmission track of the center of the fundamental frequency light beam be a straight line coincident with the twin plane of the photovoltaic photorefractive diffusion management twin; 其中,通过升降所述精密升降台使基频光在所述光伏光折变扩散管理孪晶的前端面上的聚焦光斑中心偏离孪晶面,从而使基频光在方向指向孪晶面的横向加速度作用下的光束中心传输轨迹演变成为一条周期性穿过孪晶面的蛇形曲线;Wherein, by lifting the precision lifting table, the focus spot center of the fundamental frequency light on the front face of the photovoltaic photorefractive diffusion management twin deviates from the twin plane, so that the fundamental frequency light points to the lateral direction of the twin plane The transmission trajectory of the beam center under the action of acceleration evolves into a serpentine curve that periodically passes through the twin plane; 其中,通过升降所述精密升降台来改变基频光在所述光伏光折变扩散管理孪晶的前端面上聚焦光斑的中心位置与孪晶面之间的距离,从而调节基频光在光伏光折变扩散管理孪晶内蛇形传输轨迹的弯曲程度,以使基频光和二次谐波在平行于孪晶面方向上的传播常数满足相位匹配,并能够在二次谐波输出光学器件组的输出端观测到二次谐波;其中,在观测二次谐波时,所述第二准直凸透镜,用于将从所述光伏光折变扩散管理孪晶出射的发散的包含基频光和二次谐波的混合光束准直为平行的混合光束;所述分光镜,用于将所述混合光束中的二次谐波进行反射,以及将所述混合光束中的基频光进行透射,以达到单独观测二次谐波的光强变化;Wherein, the distance between the central position of the focused spot of the fundamental frequency light on the front face of the photovoltaic photorefractive diffusion management twin and the twin plane is changed by lifting the precision lifting table, thereby adjusting the fundamental frequency light on the photovoltaic photorefractive diffusion management twin. Photorefractive diffusion manages the bending degree of the serpentine transmission trajectory in the twin, so that the propagation constants of the fundamental frequency light and the second harmonic in the direction parallel to the twin plane meet the phase matching, and the second harmonic output optical The second harmonic is observed at the output end of the device group; wherein, when observing the second harmonic, the second collimating convex lens is used to convert the divergent containing base emitted from the photovoltaic photorefractive diffusion management twin The mixed light beam of frequency light and second harmonic is collimated into a parallel mixed light beam; the beam splitter is used for reflecting the second harmonic in the mixed light beam, and for Transmission is performed to observe the light intensity change of the second harmonic alone; 其中,对所述二次谐波产生装置的运行状态进行调控和优化,以使基频光和二次谐波相干叠加组成的所述混合光束在所述光伏光折变扩散管理孪晶内形成稳定的双色亮光伏光折变空间孤子,并使二次谐波产生达到尽可能大的转换效率。Wherein, the operating state of the second harmonic generation device is regulated and optimized, so that the mixed light beam composed of the fundamental frequency light and the second harmonic coherently superimposed is formed in the photovoltaic photorefractive diffusion management twin Stable two-color bright photovoltaic photorefractive space soliton, and make the second harmonic generation achieve the largest possible conversion efficiency. 2.根据权利要求1所述的二次谐波产生装置,其特征在于:2. The second harmonic generation device according to claim 1, characterized in that: 当所述两块相同材料的光伏光折变晶体的有效载流子均为电子时,所述两块相同材料的光伏光折变晶体的负c面经光学抛光后紧密粘接在一起从而形成电子型的光伏光折变扩散管理孪晶;When the effective carriers of the two photovoltaic photorefractive crystals of the same material are electrons, the negative c- sides of the two photovoltaic photorefractive crystals of the same material are closely bonded together after optical polishing to form Electronic photovoltaic photorefractive diffusion management twinning; 当所述两块相同材料的光伏光折变晶体的有效载流子均为空穴时,所述两块相同材料的光伏光折变晶体的正c面经光学抛光后紧密粘接在一起从而形成空穴型的光伏光折变扩散管理孪晶。When the effective carriers of the two photovoltaic photorefractive crystals of the same material are both holes, the front c -planes of the two photovoltaic photorefractive crystals of the same material are optically polished and tightly bonded together so that Formation of hole-type photovoltaic photorefractive diffusion-managed twins. 3.根据权利要求2所述的二次谐波产生装置,其特征在于:3. The second harmonic generation device according to claim 2, characterized in that: 所述电子型的光伏光折变扩散管理孪晶在孪晶面的两边具有相反的载流子扩散效应;The electron-type photovoltaic photorefractive diffusion management twin has opposite carrier diffusion effects on both sides of the twin plane; 所述空穴型的光伏光折变扩散管理孪晶在孪晶面的两边具有相反的载流子扩散效应。The hole-type photovoltaic photorefractive diffusion management twin has opposite carrier diffusion effects on both sides of the twin plane. 4.一种基于光伏光折变扩散管理孪晶的二次谐波产生方法,其特征在于,所述光伏光折变扩散管理孪晶由两块相同材料的光伏光折变晶体沿一个公共晶面镜面对称耦合而成,所述方法包括:4. A second harmonic generation method based on photovoltaic photorefractive diffusion management twins, characterized in that the photovoltaic photorefractive diffusion management twins are composed of two photovoltaic photorefractive crystals of the same material along a common crystal Surface-mirror surface symmetric coupling, the method includes: 利用亮光伏光折变空间孤子在孪晶内的孪晶面处诱导出以孪晶面为中轴面的晶内条形柔性光波导,以使通过调节基频光和二次谐波在所述波导中的传播常数来实现相位匹配,从而实现二次谐波的高效产生;Using bright photovoltaic photorefractive spatial solitons to induce an intragranular strip-shaped flexible optical waveguide with the twin plane as the central axis plane at the twin plane in the twin crystal, so that by adjusting the fundamental frequency light and the second harmonic The propagation constant in the waveguide is used to achieve phase matching, so as to realize the efficient generation of the second harmonic; 所述方法还包括:The method also includes: 将所述光伏光折变扩散管理孪晶放置在精密升降台上,并使所述光伏光折变扩散管理孪晶的孪晶面平行于水平面,以及调节所述光伏光折变扩散管理孪晶的垂直高度;placing the photovoltaic photorefractive diffusion management twins on a precision lifting platform, making the twin planes of the photovoltaic photorefractive diffusion management twins parallel to the horizontal plane, and adjusting the photovoltaic photorefractive diffusion management twins the vertical height of 二次谐波产生装置包括基频光输入光学器件组、二次谐波输出光学器件组以及背景光双向照明光学器件组,其中:The second harmonic generating device includes a fundamental frequency light input optical device group, a second harmonic output optical device group and a background light bidirectional illumination optical device group, wherein: 所述基频光输入光学器件组包括基频光源、第一准直凸透镜、第一起偏器和聚焦凸透镜;The fundamental frequency light input optical device group includes a fundamental frequency light source, a first collimating convex lens, a first polarizer and a focusing convex lens; 所述二次谐波输出光学器件组包括第二准直凸透镜和分光镜;The second harmonic output optical device group includes a second collimating convex lens and a beam splitter; 所述背景光双向照明光学器件组包括背景光源、第三准直凸透镜、第二起偏器、半透半反镜、前向照明反射镜、全反镜和背向照明反射镜;The background light two-way illumination optical device group includes a background light source, a third collimating convex lens, a second polarizer, a half mirror, a forward illumination reflector, a total reflection mirror and a back illumination reflector; 所述方法还包括:The method also includes: 利用背景光源提供非相干的背景光;Use background light sources to provide incoherent background lighting; 通过第三准直凸透镜将发散的背景光准直为平行光;Collimating the divergent background light into parallel light through the third collimating convex lens; 通过第二起偏器将准直后的背景光变为偏振方向平行于所述光伏光折变扩散管理孪晶的孪晶面的线偏振光;changing the collimated background light into linearly polarized light whose polarization direction is parallel to the twin plane of the photovoltaic photorefractive diffusion management twin through the second polarizer; 通过半透半反镜将起偏后的背景光平均分成强度相等的前向照明光和背向照明光;The polarized background light is evenly divided into forward lighting and back lighting with equal intensity through the half mirror; 通过前向照明反射镜将所述前向照明光反射到所述光伏光折变扩散管理孪晶的前端面;reflecting the forward illumination light onto the front face of the photovoltaic photorefractive diffusion management twin via a forward illumination mirror; 利用全反镜改变所述背向照明光的方向;Utilizing a total reflection mirror to change the direction of the backlighting light; 通过背向照明反射镜将变向后的背向照明光反射到所述光伏光折变扩散管理孪晶的后端面,以使强度相等的前向照明光和背向照明光在所述光伏光折变扩散管理孪晶内相互平行且对向传输,使得叠加在一起的前向照明光和背向照明光对所述光伏光折变扩散管理孪晶进行双向均匀照射;The reversed back-illumination light is reflected to the rear end face of the photovoltaic photorefractive diffusion management twin through the back-illumination reflector, so that the forward and back illumination lights with equal intensities The refractive diffusion management twins are parallel to each other and transmitted in opposite directions, so that the superimposed forward illumination light and back illumination light illuminate the photovoltaic photorefractive diffusion management twins bidirectionally and uniformly; 利用基频光源提供相干的基频光;Using a fundamental frequency light source to provide coherent fundamental frequency light; 通过第一准直凸透镜将发散的基频光准直为平行光束;collimating the divergent fundamental frequency light into a parallel beam through the first collimating convex lens; 通过第一起偏器将准直后的基频光变为偏振方向垂直于所述光伏光折变扩散管理孪晶的孪晶面的线偏振光;Transforming the collimated fundamental frequency light into linearly polarized light whose polarization direction is perpendicular to the twin plane of the photovoltaic photorefractive diffusion management twin through the first polarizer; 通过聚焦凸透镜将起偏后的基频光聚焦于所述光伏光折变扩散管理孪晶的前端面上并使聚焦光斑对称分布于孪晶面的两侧;Focusing the polarized fundamental frequency light on the front face of the photovoltaic photorefractive diffusion management twin through a focusing convex lens and making the focused light spots symmetrically distributed on both sides of the twin plane; 通过改变所述背景光源的输出功率来改变所述前向照明光和背向照明光的强度,从而调节所述光伏光折变扩散管理孪晶内的光伏光折变效应的强度和响应时间;changing the intensity of the forward illumination light and the back illumination light by changing the output power of the background light source, thereby adjusting the intensity and response time of the photovoltaic photorefractive effect in the photovoltaic photorefractive diffusion management twin; 通过改变所述基频光源的输出功率以及所述聚焦凸透镜与所述光伏光折变扩散管理孪晶之间的距离来调节基频光在所述光伏光折变扩散管理孪晶的前端面上聚焦光斑的光强和尺寸,从而调节所述基频光在所述光伏光折变扩散管理孪晶内所受到的光伏光折变非线性自聚焦效应,直至使基频光的自聚焦效应补偿其衍射展宽效应,以使基频光在所述光伏光折变扩散管理孪晶内实现无衍射传输,即基频光在所述光伏光折变扩散管理孪晶内实现亮光伏光折变空间孤子传输,并使基频光光束中心的传输轨迹是一条与所述光伏光折变扩散管理孪晶的孪晶面相重合的直线;Adjusting the fundamental frequency light on the front face of the photovoltaic photorefractive diffusion management twin by changing the output power of the fundamental frequency light source and the distance between the focusing convex lens and the photovoltaic photorefractive diffusion management twin focusing the light intensity and size of the light spot, thereby adjusting the photovoltaic photorefractive nonlinear self-focusing effect suffered by the fundamental frequency light in the photovoltaic photorefractive diffusion management twin, until the self-focusing effect of the fundamental frequency light is compensated Its diffraction broadening effect enables the fundamental frequency light to realize non-diffraction transmission in the photovoltaic photorefractive diffusion management twin, that is, the fundamental frequency light realizes bright photovoltaic photorefractive space in the photovoltaic photorefractive diffusion management twin Soliton transmission, and make the transmission track of the center of the fundamental frequency light beam be a straight line coincident with the twin plane of the photovoltaic photorefractive diffusion management twin; 其中,通过升降所述精密升降台使基频光在所述光伏光折变扩散管理孪晶的前端面上的聚焦光斑中心偏离孪晶面,从而使基频光在方向指向孪晶面的横向加速度作用下的光束中心传输轨迹演变成为一条周期性穿过孪晶面的蛇形曲线;Wherein, by lifting the precision lifting table, the focus spot center of the fundamental frequency light on the front face of the photovoltaic photorefractive diffusion management twin deviates from the twin plane, so that the fundamental frequency light points to the lateral direction of the twin plane The transmission trajectory of the beam center under the action of acceleration evolves into a serpentine curve that periodically passes through the twin plane; 其中,通过升降所述精密升降台来改变基频光在所述光伏光折变扩散管理孪晶的前端面上聚焦光斑的中心位置与孪晶面之间的距离,从而调节基频光在光伏光折变扩散管理孪晶内蛇形传输轨迹的弯曲程度,以使基频光和二次谐波在平行于孪晶面方向上的传播常数满足相位匹配,并达到在二次谐波输出光学器件组的输出端观测到二次谐波;其中,在观测二次谐波时,所述第二准直凸透镜,用于将从所述光伏光折变扩散管理孪晶出射的发散的包含基频光和二次谐波的混合光束准直为平行的混合光束;所述分光镜,用于将所述混合光束中的二次谐波进行反射,以及将所述混合光束中的基频光进行透射,以达到单独观测二次谐波的光强变化;Wherein, the distance between the central position of the focused spot of the fundamental frequency light on the front face of the photovoltaic photorefractive diffusion management twin and the twin plane is changed by lifting the precision lifting table, thereby adjusting the fundamental frequency light on the photovoltaic photorefractive diffusion management twin. Photorefractive diffusion manages the bending degree of the serpentine transmission trajectory in the twin, so that the propagation constants of the fundamental frequency light and the second harmonic in the direction parallel to the twin plane meet the phase matching, and achieve optical The second harmonic is observed at the output end of the device group; wherein, when observing the second harmonic, the second collimating convex lens is used to convert the divergent containing base emitted from the photovoltaic photorefractive diffusion management twin The mixed light beam of frequency light and second harmonic is collimated into a parallel mixed light beam; the beam splitter is used for reflecting the second harmonic in the mixed light beam, and for Transmission is performed to observe the light intensity change of the second harmonic alone; 其中,对所述二次谐波产生装置的运行状态进行调控和优化,以使基频光和二次谐波相干叠加组成的所述混合光束在所述光伏光折变扩散管理孪晶内形成稳定的双色亮光伏光折变空间孤子,并使二次谐波产生达到尽可能大的转换效率。Wherein, the operating state of the second harmonic generation device is regulated and optimized, so that the mixed light beam composed of the fundamental frequency light and the second harmonic coherently superimposed is formed in the photovoltaic photorefractive diffusion management twin Stable two-color bright photovoltaic photorefractive space soliton, and make the second harmonic generation achieve the largest possible conversion efficiency. 5.根据权利要求4所述的二次谐波产生方法,其特征在于:当所述两块相同材料的光伏光折变晶体的有效载流子均为电子时,所述两块相同材料的光伏光折变晶体的负c面经光学抛光后紧密粘接在一起从而形成电子型的光伏光折变扩散管理孪晶;当所述两块相同材料的光伏光折变晶体的有效载流子均为空穴时,所述两块相同材料的光伏光折变晶体的正c面经光学抛光后紧密粘接在一起从而形成空穴型的光伏光折变扩散管理孪晶。5. The second harmonic generation method according to claim 4, characterized in that: when the effective carriers of the photovoltaic photorefractive crystals of the two identical materials are electrons, the The negative c- sides of the photovoltaic photorefractive crystals are closely bonded together after optical polishing to form electronic photovoltaic photorefractive diffusion management twins; when the effective carriers of the two photovoltaic photorefractive crystals of the same material When both are holes, the front c -planes of the two photovoltaic photorefractive crystals of the same material are optically polished and closely bonded together to form hole-type photovoltaic photorefractive diffusion management twins. 6.根据权利要求5所述的二次谐波产生方法,其特征在于:所述电子型的光伏光折变扩散管理孪晶在孪晶面的两边具有相反的载流子扩散效应;所述空穴型的光伏光折变扩散管理孪晶在孪晶面的两边具有相反的载流子扩散效应。6. The second harmonic generation method according to claim 5, characterized in that: the electron-type photovoltaic photorefractive diffusion management twin has opposite carrier diffusion effects on both sides of the twin plane; Hole-type photovoltaic photorefractive diffusion-managed twins have opposite carrier diffusion effects on both sides of the twin plane.
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