技术领域technical field
本实用新型涉及光学技术领域，更具体地，涉及一种铌酸锂晶体结合结构和一种高能太赫兹脉冲产生装置。The utility model relates to the field of optical technology, in particular to a lithium niobate crystal bonding structure and a high-energy terahertz pulse generating device.
背景技术Background technique
太赫兹(THz)辐射通常指的是从0.1～10THz的电磁波，其波段在微波和远红外之间。由于太赫兹频率在电磁波谱上的特殊位置，使得这个频段的高能量光源非常缺乏。高能量的太赫兹辐射源按照装置的大小可分为同步辐射太赫兹源和桌面式小型太赫兹源。同步辐射的太赫兹源可产生百微焦量级的太赫兹脉冲，但这样的大型装置耗资巨大且运行昂贵。桌面式的强场太赫兹辐射源主要由脉冲飞秒激光器驱动，按照产生方式的不同可分为：光学整流、光导天线、空气等离子体、激光打靶等。Terahertz (THz) radiation usually refers to electromagnetic waves from 0.1 to 10 THz, and its wave band is between microwave and far infrared. Due to the special position of terahertz frequency on the electromagnetic spectrum, high-energy light sources in this frequency band are very scarce. According to the size of the device, high-energy terahertz radiation sources can be divided into synchrotron radiation terahertz sources and desktop small terahertz sources. Terahertz sources for synchrotron radiation can produce terahertz pulses on the order of hundreds of microjoules, but such large devices are expensive and expensive to run. Desktop strong-field terahertz radiation sources are mainly driven by pulsed femtosecond lasers, which can be divided into optical rectification, photoconductive antenna, air plasma, laser targeting, etc. according to different generation methods.
尽管激光打靶已经获得了几百微焦的能量，但是激光打靶所获得的太赫兹辐射的方向性差，不适合后续应用，且辐射效率较低，辐射机理也有待进一步研究。空气等离子体产生的太赫兹可以获得超宽带的辐射，对材料的表征非常有优势，而且空气作为非线性介质不存在损伤阈值问题，但这种方法所产生的太赫兹辐射效率低，空气等离子体不稳定，系统的信噪比差，对双色的相位匹配要求高，机理也还有待进一步探索。大孔径光电导天线辐射的太赫兹效率高，稳定性好，覆盖了太赫兹辐射的低频段，但光电导天线依赖外加直流电场和高激发功率，会导致天线击穿和载流子的屏蔽效应，因此天线容易破坏，且获得的绝对太赫兹能量相对较低。Although laser targeting has obtained hundreds of microjoules of energy, the terahertz radiation obtained by laser targeting has poor directivity, which is not suitable for subsequent applications, and the radiation efficiency is low, and the radiation mechanism needs further study. The terahertz radiation generated by air plasma can obtain ultra-broadband radiation, which is very advantageous for the characterization of materials, and air does not have the problem of damage threshold as a nonlinear medium, but the terahertz radiation generated by this method has low efficiency, and air plasma Unstable, the signal-to-noise ratio of the system is poor, and the requirements for phase matching of two colors are high, and the mechanism needs to be further explored. The terahertz radiation of large-aperture photoconductive antennas has high efficiency and good stability, and covers the low frequency band of terahertz radiation. However, photoconductive antennas rely on external DC electric fields and high excitation power, which will lead to antenna breakdown and carrier shielding effects. , so the antenna is easily damaged, and the absolute terahertz energy obtained is relatively low.
到目前为止，光学整流是被认为最有效的桌面式产生强场太赫兹辐射的方法。在利用光学整流产生太赫兹辐射的过程中，同一个红外光脉冲包罗中的不同光谱分量之间产生级联差频过程，实现太赫兹辐射的产生。只要相位匹配条件得到满足，该频率下转换的过程将会级联的反复发生，有可能使得红外光子完全转换为多个太赫兹光子，获得>100％光子转换效率。碲化锌(ZnTe)和磷化镓(GaP)一直是被用来通过光学整流实现太赫兹源常见的材料。由于它们的非线性系数不够高且在红外频率有极大的双光子吸收，研究人员已经把目光转向非线性系数较大的有机晶体和铌酸锂(LiNbO3)晶体。虽然有机晶体很被看好，它所固有的缺点，例如低破坏阈值，无法用于高功率高能量激光器；小尺寸，无法用于高能量大光斑的激光器激发；材料不稳定，易于潮解，无法制备牢固的太赫兹发射源；需要特定的波长 1.2μm-1.5μm泵浦，而该频段的高能量激光器的技术不够成熟；晶体价格非常昂贵等，使得利用有机晶体来产生强场太赫兹脉冲让人望而却步。So far, optical rectification is considered the most efficient way to generate strong-field terahertz radiation on a tabletop basis. In the process of using optical rectification to generate terahertz radiation, a cascade difference frequency process is generated between different spectral components contained in the same infrared light pulse to realize the generation of terahertz radiation. As long as the phase-matching condition is satisfied, the frequency down-conversion process will occur repeatedly in cascade, and it is possible to completely convert infrared photons into multiple terahertz photons and obtain >100% photon conversion efficiency. Zinc telluride (ZnTe) and gallium phosphide (GaP) have been common materials used to realize terahertz sources through optical rectification. Because their nonlinear coefficients are not high enough and they have great two-photon absorption at infrared frequencies, researchers have turned their attention to organic crystals and lithium niobate (LiNbO3) crystals with larger nonlinear coefficients. Although organic crystals are very promising, their inherent shortcomings, such as low damage threshold, cannot be used for high-power high-energy lasers; small size, cannot be used for high-energy and large-spot laser excitation; materials are unstable, easy to deliquescence, and cannot be prepared Strong terahertz emission source; specific wavelength 1.2μm-1.5μm pump is required, and the technology of high-energy lasers in this frequency band is not mature enough; crystals are very expensive, etc., making the use of organic crystals to generate strong-field terahertz pulses exciting Stay away.
第二种方法利用光学整流的方法是利用倾斜波前技术在铌酸锂晶体中产生强场太赫兹辐射。铌酸锂在光学领域的地位相当于硅材料在半导体工业，是一个很好的候选材料。它具有非常多的优点，比如大的损伤阈值，可用于高能量激光器；高非线性系数，可获得高的能量转化效率；大的能量带隙(4eV)，克服双光子或多光子吸收带来的能量损耗；对泵浦波长无选择性等。但由于红外光和太赫兹波在铌酸锂晶体中有着不同的折射率，前者约为5，后者约为2.3，为了能够实现最大限度的相位匹配，Hebling等提出了倾斜波前的方法参见非专利文献美国光学快报Optics Express，10卷，第21期，1611-1166页。The second approach to exploit optical rectification is to generate strong-field terahertz radiation in lithium niobate crystals using the tilted wavefront technique. The status of lithium niobate in the optical field is equivalent to that of silicon materials in the semiconductor industry, and it is a good candidate material. It has many advantages, such as a large damage threshold, which can be used in high-energy lasers; a high nonlinear coefficient, which can obtain high energy conversion efficiency; a large energy band gap (4eV), which can overcome the problems caused by two-photon or multi-photon absorption. energy loss; no selectivity to the pump wavelength, etc. However, since infrared light and terahertz waves have different refractive indices in lithium niobate crystals, the former is about 5, and the latter is about 2.3. In order to achieve maximum phase matching, Hebling et al. proposed a method of tilting the wavefront, see Non-Patent Literature Optics Express, Vol. 10, No. 21, pp. 1611-1166.
现有技术中，使用光子学方法产生太赫兹波的关键步骤在于铌酸锂发射晶体的切割方式采用梯形或等腰三角形的切割方式。在实验过程中，激发光直接照射在晶体的62-63°角，太赫兹波则沿着与入射激发光成一个角度方向发射出来。In the prior art, the key step of using photonics method to generate terahertz wave is that the cutting method of lithium niobate emitting crystal adopts trapezoidal or isosceles triangular cutting method. During the experiment, the excitation light is directly irradiated on the crystal at an angle of 62-63°, and the terahertz wave is emitted along a direction at an angle to the incident excitation light.
在现有技术中，由于倾斜波前技术在空间几何上的非共线特征，使得当高能量(单脉冲能量高于100mJ)、大光斑(光斑直径大于5mm) 的飞秒激光脉冲作用在铌酸锂晶体上产生高能太赫兹脉冲的时候，靠近晶体62-63°角切割边沿的激发光在晶体内传播距离过短，而远离该角边沿的激发光在晶体内传播距离长，这就使得激发光到太赫兹波的光子能量转化效率无法进一步提高，甚至保持在原有水平都很困难。In the prior art, due to the non-collinear feature of the inclined wavefront technology in spatial geometry, when femtosecond laser pulses with high energy (single pulse energy higher than 100mJ) and large spot (spot diameter greater than 5mm) act on niobium When a high-energy terahertz pulse is generated on a lithium oxide crystal, the excitation light close to the 62-63° angle cutting edge of the crystal has a too short propagation distance in the crystal, while the excitation light far away from the angle edge has a long propagation distance in the crystal, which makes The photon energy conversion efficiency from excitation light to terahertz waves cannot be further improved, and it is even difficult to maintain at the original level.
实用新型内容Utility model content
为解决现有技术中飞秒激光脉冲作用在铌酸锂晶体上产生高能太赫兹脉冲的时候，靠近晶体62-63°角切割边沿的激发光在晶体内传播距离过短，而远离该角边沿的激发光在晶体内传播距离长，这就使得激发光到太赫兹波的光子能量转化效率无法进一步提高的问题，提出一种铌酸锂晶体结合结构和一种高能太赫兹脉冲产生装置。In order to solve the problem that when femtosecond laser pulses act on lithium niobate crystals to generate high-energy terahertz pulses in the prior art, the excitation light close to the 62-63° angle cutting edge of the crystal travels too short in the crystal, and far away from the angle edge The long propagation distance of the excitation light in the crystal makes it impossible to further improve the photon energy conversion efficiency from the excitation light to the terahertz wave. A lithium niobate crystal combined structure and a high-energy terahertz pulse generating device are proposed.
根据本实用新型的一个方面，提供一种铌酸锂晶体结合结构，包括：底角为62～63度，顶角为54～56度的等腰三角形棱柱铌酸锂晶体以及一个厚度为1～5mm的铌酸锂晶片，所述铌酸锂晶片通过光学接触的方法完全覆盖于所述等腰三角形棱柱铌酸锂晶体底边所在的柱面上；According to one aspect of the present invention, a lithium niobate crystal bonding structure is provided, comprising: an isosceles triangular prism lithium niobate crystal with a base angle of 62-63 degrees and an apex angle of 54-56 degrees and a lithium niobate crystal with a thickness of 1-60 degrees. 5mm lithium niobate wafer, the lithium niobate wafer completely covers the cylindrical surface where the bottom edge of the isosceles triangular prism lithium niobate crystal is located by the method of optical contact;
其中，所述等腰三角形棱柱铌酸锂晶体的三个柱面经过光学抛光处理。Wherein, the three cylindrical surfaces of the isosceles triangular prism lithium niobate crystal are optically polished.
其中，所述铌酸锂晶体结合结构中掺杂有5～6.2mol％的氧化镁。Wherein, the lithium niobate crystal bonding structure is doped with 5-6.2 mol% magnesium oxide.
根据本实用新型的第二方面，提供一种高能太赫兹脉冲产生装置，包括：飞秒激光器、反射光栅、半波片、成像透镜和一个如本实用新型第一方面提供的铌酸锂晶体结合结构，所述飞秒激光器发射的泵浦飞秒激光通过所述反射光栅衍射到所述半波片上，经过所述半波片改变所述泵浦飞秒激光的偏振方向后，再通过成像透镜后入射至铌酸锂晶体结合结构中，从而在所述铌酸锂晶片中产生太赫兹脉冲辐射。According to the second aspect of the utility model, a high-energy terahertz pulse generating device is provided, including: a femtosecond laser, a reflective grating, a half-wave plate, an imaging lens and a combination of lithium niobate crystal as provided in the first aspect of the utility model structure, the pumping femtosecond laser emitted by the femtosecond laser is diffracted onto the half-wave plate through the reflection grating, and after the polarization direction of the pumping femtosecond laser is changed by the half-wave plate, it passes through the imaging lens Then, it is incident into the lithium niobate crystal bonding structure, thereby generating terahertz pulsed radiation in the lithium niobate wafer.
其中，所述反射光栅的刻线密度为1500～2000线每毫米。Wherein, the groove density of the reflective grating is 1500-2000 lines per millimeter.
其中，所述光栅和所述铌酸锂晶体之间的成像透镜为单个透镜、双透镜组合或柱透镜组合；所述成像透镜的成像倍数为0.3～0.6倍。Wherein, the imaging lens between the grating and the lithium niobate crystal is a single lens, a double lens combination or a cylindrical lens combination; the imaging magnification of the imaging lens is 0.3-0.6 times.
其中，所述泵浦飞秒激光入射到所述铌酸锂晶体结合结构时的所述泵浦飞秒激光的偏振方向与所述铌酸锂晶片的晶轴平行。Wherein, when the pumping femtosecond laser light is incident on the lithium niobate crystal bonding structure, the polarization direction of the pumping femtosecond laser light is parallel to the crystal axis of the lithium niobate wafer.
本实用新型提出的一种高能太赫兹脉冲产生装置，通过改进铌酸锂晶体的结构，对于高能量、大光斑的激发光可以维持高效率的太赫兹辐射，同时射的太赫兹波不存在非线性失真的问题，获得更好的太赫兹波发射特性，便于后续实验应用。A high-energy terahertz pulse generating device proposed by the utility model can maintain high-efficiency terahertz radiation for high-energy and large-spot excitation light by improving the structure of lithium niobate crystals, and the terahertz waves emitted at the same time do not have abnormal To solve the problem of linear distortion, better terahertz wave emission characteristics are obtained, which is convenient for subsequent experimental applications.
附图说明Description of drawings
图1为本实用新型一实施例提供的一种用于产生高能太赫兹脉冲的铌酸锂晶体结合结构中等腰三角形棱柱铌酸锂晶体设计的结构图；Fig. 1 is a structural diagram of an isosceles triangular prism lithium niobate crystal design in a lithium niobate crystal bonding structure for generating high-energy terahertz pulses provided by an embodiment of the present invention;
图2为本实用新型一实施例提供的一种用于产生高能太赫兹脉冲的铌酸锂晶体结合结构的俯视图；Fig. 2 is a top view of a lithium niobate crystal bonding structure for generating high-energy terahertz pulses provided by an embodiment of the present invention;
图3为本实用新型另一实施例提供的一种高能太赫兹脉冲产生装置的结构图；Fig. 3 is a structural diagram of a high-energy terahertz pulse generating device provided by another embodiment of the present invention;
图4为本实用新型另一实施例提供的一种高能太赫兹脉冲产生装置的光路图。Fig. 4 is an optical path diagram of a high-energy terahertz pulse generating device provided by another embodiment of the present invention.
具体实施方式Detailed ways
下面结合附图和实施例，对本实用新型的具体实施方式作进一步详细描述。以下实施例用于说明本实用新型，但不用来限制本实用新型的范围。Below in conjunction with accompanying drawing and embodiment, the specific embodiment of the utility model is described in further detail. The following examples are used to illustrate the utility model, but not to limit the scope of the utility model.
参考图1和图2，图1为本实用新型一实施例提供的一种用于产生高能太赫兹脉冲的铌酸锂晶体结合结构中等腰三角形棱柱铌酸锂晶体的结构图；图2为本实用新型一实施例提供的一种用于产生高能太赫兹脉冲的铌酸锂晶体结合结构的俯视图。所述铌酸锂晶体结合结构具体包括：With reference to Fig. 1 and Fig. 2, Fig. 1 is a structure diagram of an isosceles triangular prism lithium niobate crystal in a lithium niobate crystal bonding structure used to generate high-energy terahertz pulses provided by an embodiment of the present invention; Fig. 2 is the structure diagram of this utility model A plan view of a lithium niobate crystal bonding structure for generating high-energy terahertz pulses provided by an embodiment of the utility model. The lithium niobate crystal binding structure specifically includes:
切割成底角为62～63度，顶角为54～56度的等腰三角形棱柱铌酸锂晶体以及一个厚度为1～5mm的铌酸锂晶片，所述铌酸锂晶片通过光学接触的方法完全覆盖于所述等腰三角形棱柱铌酸锂晶体底边所在的柱面上，其中，所述等腰三角形棱柱铌酸锂晶体的三个柱面经过光学抛光处理。Cutting into an isosceles triangular prism lithium niobate crystal with a base angle of 62-63 degrees and a top angle of 54-56 degrees and a lithium niobate wafer with a thickness of 1-5 mm, the lithium niobate wafer is optically contacted It completely covers the cylindrical surface where the base of the isosceles triangular prism lithium niobate crystal is located, wherein the three cylindrical surfaces of the isosceles triangular prism lithium niobate crystal are optically polished.
具体的，沿着晶体的Y方向切割的铌酸锂等腰三角棱形晶体；该晶体在XZ平面内的切割方式为两个底角62.8度、顶角54.4度的等腰三角形；Y方向切割的铌酸锂棱镜为6.0mol％的MgO掺杂浓度。它为三角形结构。三个长方形表面未镀增透膜。在晶体XZ平面内的两等腰三角形面无需抛光，而对于与Y轴方向平行的三个面需光学抛光。该铌酸锂棱形晶体的作用在于，将入射激光倾斜的波前通过成功传输到结合的铌酸锂晶片上，并将产生了太赫兹辐射后的生物激发光能量成功的全反射出来，以便用于下一级太赫兹辐射的产生，达到激发光能量反复使用的目的，以提高太赫兹辐射的能量转化效率。Specifically, an isosceles triangular prism crystal of lithium niobate cut along the Y direction of the crystal; the cutting method of the crystal in the XZ plane is two isosceles triangles with a base angle of 62.8 degrees and an apex angle of 54.4 degrees; cutting in the Y direction The lithium niobate prisms have a MgO doping concentration of 6.0 mol%. It is a triangular structure. The three rectangular surfaces are not AR coated. The two isosceles triangular faces in the XZ plane of the crystal do not need to be polished, but the three faces parallel to the Y-axis direction need to be optically polished. The role of the lithium niobate prismatic crystal is to successfully transmit the inclined wavefront of the incident laser light to the combined lithium niobate wafer, and to completely reflect the bio-excited light energy after the terahertz radiation is generated, so that It is used for the generation of next-level terahertz radiation to achieve the purpose of repeated use of excitation light energy, so as to improve the energy conversion efficiency of terahertz radiation.
在该晶体的54.4度角正对的平面上，通过光学接触的方法需紧密结合一块铌酸锂晶片，该晶片的切割方式为Y方向切割；晶片的Z轴方向与晶体的Y轴平行；晶片的大小需完全覆盖铌酸锂棱形晶体的等腰三角形底边所在的面，且该晶片的X轴与铌酸锂棱形晶体的Y轴垂直。通过铌酸锂棱形晶体后的激发光可顺利传输到铌酸锂晶片中，在结合的面内不会造成反射损失，也不会对倾斜波前造成破坏而使得高能太赫兹脉冲无法产生。On the plane facing the crystal at an angle of 54.4 degrees, a lithium niobate wafer needs to be tightly bonded by optical contact, and the cutting method of the wafer is Y-direction cutting; the Z-axis direction of the wafer is parallel to the Y-axis of the crystal; The size of the wafer needs to completely cover the face where the base of the isosceles triangle of the lithium niobate prismatic crystal is located, and the X axis of the wafer is perpendicular to the Y axis of the lithium niobate prismatic crystal. The excitation light passing through the lithium niobate prismatic crystal can be smoothly transmitted to the lithium niobate wafer, without causing reflection loss in the combined plane, and will not cause damage to the inclined wavefront, so that high-energy terahertz pulses cannot be generated.
其中，所述铌酸锂晶体结合结构掺杂有5～6.2mol％的氧化镁。Wherein, the lithium niobate crystal bonding structure is doped with 5-6.2 mol% magnesium oxide.
通过此铌酸锂晶体结合结构，对于高能量、大光斑的激发光，克服传统晶体结构无法维持高效率的太赫兹辐射的问题，同时特殊的设计使得出射的太赫兹波不存在非线性失真的问题，获得更好的太赫兹波发射特性，便于后续实验应用。Through this lithium niobate crystal combined structure, for high-energy and large-spot excitation light, the problem that the traditional crystal structure cannot maintain high-efficiency terahertz radiation is overcome, and the special design makes the emitted terahertz wave free of nonlinear distortion. To solve the problem, better terahertz wave emission characteristics are obtained, which is convenient for subsequent experimental applications.
参考图3，图3为本实用新型另一实施例提供的一种高能太赫兹脉冲产生装置的结构图，所述装置包括：飞秒激光器31、反射光栅32、半波片33、成像透镜34和铌酸锂晶体结合结构35。Referring to FIG. 3, FIG. 3 is a structural diagram of a high-energy terahertz pulse generating device provided by another embodiment of the present invention, the device includes: a femtosecond laser 31, a reflective grating 32, a half-wave plate 33, and an imaging lens 34 and lithium niobate crystal bound structure 35.
所述飞秒激光器31发射的泵浦飞秒激光通过所述反射光栅32衍射到所述半波片33上，经过所述半波片33改变所述泵浦飞秒激光的偏振方向后，再通过成像透镜34后入射至铌酸锂晶体结合结构35中，从而在所述铌酸锂晶片中产生太赫兹脉冲辐射。The pumping femtosecond laser light emitted by the femtosecond laser 31 is diffracted onto the half-wave plate 33 through the reflection grating 32, and after the half-wave plate 33 changes the polarization direction of the pumping femtosecond laser light, then After passing through the imaging lens 34, it is incident into the lithium niobate crystal bonding structure 35, thereby generating terahertz pulsed radiation in the lithium niobate wafer.
具体的，参考图4，图4为本实用新型另一实施例提供的一种高能太赫兹脉冲产生装置的光路图，本实施例采用重复频率为10Hz-1kHz，中心波长为800nm-2000nm的放大级激光器41产生的激光脉冲来激发上述实施例提供的铌酸锂晶体结合结构45，激发光脉冲宽度为 50fs-1ps，单脉冲最高能量约mJ量级，光斑直径为5.6mm*5.3mm。激发光脉冲通过1500-2000刻线每毫米的光栅42衍射到半波片上，通过精确计算光栅的入射角与衍射角，这里利用一个半波片43将光的偏振方向从水平转向竖直，并与绑定的铌酸锂晶片的光轴方向平行，使得对于晶片结合结构，产生太赫兹脉冲辐射位于被绑定的晶片内，而非三角形切割的铌酸锂晶体内。光栅与晶体间的成像系统为柱透镜对44，成像缩小倍数为0.3-0.6倍。Specifically, refer to Fig. 4. Fig. 4 is an optical path diagram of a high-energy terahertz pulse generating device provided by another embodiment of the present invention. The laser pulse generated by the laser 41 is used to excite the lithium niobate crystal bonding structure 45 provided in the above embodiment. The pulse width of the excitation light is 50fs-1ps, the maximum energy of a single pulse is about the order of mJ, and the diameter of the spot is 5.6mm*5.3mm. The excitation light pulse is diffracted onto the half-wave plate through the grating 42 with 1500-2000 lines per millimeter. By accurately calculating the incident angle and diffraction angle of the grating, a half-wave plate 43 is used here to change the polarization direction of the light from horizontal to vertical, and It is parallel to the direction of the optical axis of the bonded lithium niobate wafer, so that for the wafer bonded structure, the terahertz pulsed radiation generated is located in the bonded wafer instead of the triangular cut lithium niobate crystal. The imaging system between the grating and the crystal is a cylindrical lens pair 44, and the imaging reduction factor is 0.3-0.6 times.
在上述实施例的基础上，优选的，所述反射光栅的刻线密度为 1500～2000线每毫米。Based on the above embodiments, preferably, the reticle density of the reflective grating is 1500-2000 lines per millimeter.
所述光栅和所述铌酸锂晶体之间的成像透镜可以为单个透镜、双透镜组合或柱透镜组合，所述成像透镜的成像倍数为0.3～0.6倍。其中，所述泵浦飞秒激光入射到所述铌酸锂晶体时的偏振方向与所述铌酸锂晶片的晶轴平行。The imaging lens between the grating and the lithium niobate crystal can be a single lens, a double lens combination or a cylindrical lens combination, and the imaging magnification of the imaging lens is 0.3-0.6 times. Wherein, when the pump femtosecond laser is incident on the lithium niobate crystal, the polarization direction is parallel to the crystal axis of the lithium niobate wafer.
通过此装置，由于竖直方向的偏振光与绑定的铌酸锂晶片的光轴方向平行，使得对于晶片结合结构，产生太赫兹脉冲辐射位于被绑定的晶片内，而非三角形切割的铌酸锂晶体内，使得对于高能量、大光斑的激发光，可以长时间维持高效率的太赫兹辐射高效率的太赫兹辐射，射的太赫兹波不存在非线性失真的问题，获得更好的太赫兹波发射特性，便于后续实验应用。Through this device, since the polarized light in the vertical direction is parallel to the optical axis direction of the bonded lithium niobate wafer, for the wafer bonded structure, the terahertz pulsed radiation is generated in the bonded wafer instead of the triangular cut niobium Lithium Oxide crystal, so that for high-energy, large-spot excitation light, high-efficiency terahertz radiation can be maintained for a long time, and the emitted terahertz wave does not have the problem of nonlinear distortion, and better Terahertz wave emission characteristics are convenient for subsequent experimental applications.
最后，本申请的方法仅为较佳的实施方案，并非用于限定本实用新型的保护范围。凡在本实用新型的精神和原则之内，所作的任何修改、等同替换、改进等，均应包含在本实用新型的保护范围之内。Finally, the method of the present application is only a preferred implementation, and is not intended to limit the protection scope of the present utility model. Any modification, equivalent replacement, improvement, etc. made within the spirit and principles of the present utility model shall be included in the protection scope of the present utility model.
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| CN201721353418.6UCN207799304U (en) | 2017-10-19 | 2017-10-19 | A kind of lithium columbate crystal integrated structure and a kind of high energy terahertz pulse generation device |
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| CN201721353418.6UCN207799304U (en) | 2017-10-19 | 2017-10-19 | A kind of lithium columbate crystal integrated structure and a kind of high energy terahertz pulse generation device |
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| CN107561815B (en)* | 2017-10-19 | 2023-09-26 | 北京航空航天大学 | A high-energy terahertz pulse generating device and method |
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