CN103149708A - Any field polarization state control system - Google Patents
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Abstract
Description
技术领域 technical field
本发明涉及一种能对任意场分布光场偏振态进行控制的光学系统。该系统能够将任意场分布光场转换为诸如非偏振光等预期偏振状态,甚至可以达到将光场的偏振状态完全消除,这将有利于诸如在ICF装置中降低光斑中的子光束干涉斑纹,从而实现对激光的束匀滑的目的。 The invention relates to an optical system capable of controlling the polarization state of an arbitrary field distribution light field. The system can convert any field distribution light field into the expected polarization state such as unpolarized light, and even completely eliminate the polarization state of the light field, which will help reduce the sub-beam interference speckle in the spot in the ICF device, for example, Thereby achieving the purpose of smoothing the laser beam.
背景技术 Background technique
对于实现惯性约束聚变(ICF,Inertial Confinement Fusion)的激光装置来说,其对聚焦在靶面光束的偏振是指光场中电场分量振动的方向与传播方向垂直。在垂直于光传播的平面上,电场分量(亦称为光矢量)有不同的振动状态,由此对应不同的偏振态。偏振态光束有诸多的实际用途。例如,卫星通信和光纤通信中采用同频率的两束正交的电磁波能使信号的传输率翻倍;生物和化学科学家利用对左旋和右旋圆偏振光吸收率的差别来检测具有对映异构体特性的化学分子或生物大分子;不同偏振态的激光光束还被用于量子密码技术中;在无创伤激光诊疗诊断技术中,偏振光成像也是很前沿的应用;在对生物组织的病理性病变的光学检测技术中,输出光场的信息中包含有场的极化参量(即偏振态)。此外,对于惯性约束聚变(ICF,Inertial Confinement Fusion)的激光装置,则需要将入射激光转换为非偏振光,达到消偏振的目的,从而有利于实现靶面的均匀辐照。目前,偏振控制器的类型很多,但原理均是通过双折射效应来使一个偏振态的两个分量产生不同的相位延迟,从而再重新生成所预期的偏振态。根据其技术原理,偏振控制器大致可分为三类:方位角控制型、延迟量控制型及方位角—延迟量控制型。但是这类偏振控制器存在很多缺点,如波片、微透镜等元件造价不菲,并且需要镀增透膜以减小反射损耗,波片对波长敏感等。后来基于相同原理的全光纤偏振控制器出现,其损耗小,造价低,但仍然对波长敏感,且控制速度慢。而液晶型、电光晶体型、压电陶瓷可变可转波片型等偏振控制器相继被提出,但都存在一些不能克服的缺点,所以对偏振控制器的研究一直在进行中。为了能够将任意光场的偏振状态转化为任意预期的偏振状态,我们提出一种全新的偏振控制系统。 For laser devices that realize inertial confinement fusion (ICF, Inertial Confinement Fusion), the polarization of the beam focused on the target surface means that the vibration direction of the electric field component in the light field is perpendicular to the propagation direction. In the plane perpendicular to the light propagation, the electric field component (also known as the light vector) has different vibration states, which correspond to different polarization states. Polarized light beams have many practical uses. For example, using two beams of orthogonal electromagnetic waves of the same frequency in satellite communication and optical fiber communication can double the transmission rate of the signal; biological and chemical scientists use the difference in the absorption rate of left-handed and right-handed circularly polarized light to detect enantiotropic Chemical molecules or biological macromolecules with conformational characteristics; laser beams of different polarization states are also used in quantum cryptography; in non-invasive laser diagnosis and treatment diagnostic technology, polarized light imaging is also a very cutting-edge application; in the pathology of biological tissues In the optical detection technology of sexual lesions, the information of the output light field contains the polarization parameter of the field (that is, the polarization state). In addition, for inertial confinement fusion (ICF, Inertial Confinement Fusion) laser devices, it is necessary to convert the incident laser light into unpolarized light to achieve the purpose of depolarization, which is beneficial to achieve uniform irradiation of the target surface. At present, there are many types of polarization controllers, but the principle is to make the two components of a polarization state produce different phase delays through the birefringence effect, so as to regenerate the expected polarization state. According to its technical principle, polarization controllers can be roughly divided into three categories: azimuth control type, delay control type and azimuth-delay control type. However, this type of polarization controller has many disadvantages, such as the high cost of components such as wave plates and microlenses, and the need for anti-reflection coatings to reduce reflection losses, and the wave plates are sensitive to wavelengths. Later, an all-fiber polarization controller based on the same principle appeared, which has small loss and low cost, but is still sensitive to wavelength and has a slow control speed. The polarization controllers such as liquid crystal type, electro-optic crystal type, and piezoelectric ceramic variable and switchable wave plate type have been proposed one after another, but there are some insurmountable shortcomings, so the research on polarization controllers has been in progress. In order to transform the polarization state of any light field into any desired polarization state, we propose a novel polarization control system.
发明内容 Contents of the invention
目前,尚未见之有关任意光场偏振状态的控制系统的报道,但是光场的偏振态在现代光学应用中是一个极为重要的物理量,诸如在ICF装置中就需要克服现有的偏振匀滑技术无法消除子光束的干涉斑纹的不足,本系统基于此而被我们所提出。本发明中的光场偏振状态控制系统能实现任意光场的偏振控制,甚至可将入射激光转换为非偏振光,从而避免光束在聚焦时发生子光束的干涉,从而达到束匀滑的目的。 At present, there is no report on the control system of the polarization state of the arbitrary light field, but the polarization state of the light field is an extremely important physical quantity in modern optical applications, such as in the ICF device, it is necessary to overcome the existing polarization smoothing technology The deficiency of the interference pattern of the sub-beams cannot be eliminated, and this system is proposed by us based on this. The light field polarization state control system in the present invention can realize the polarization control of any light field, and even convert the incident laser light into non-polarized light, so as to avoid the interference of sub-beams when the light beam is focused, so as to achieve the purpose of beam smoothness.
本发明的技术方案是:在系统装置中有一块光场偏振态控制阵列板,该板起到偏振控制的作用,由p×q个处理单元构成,每一个单元安置一个可控电光晶体,如KDP晶体。通过加上适当的电压使电光晶体片对入射偏振光的两个分量产生适合的位相延迟,从而使出射光成为我们所需要的偏振光,达到调制入射光束偏振态的目的。当激光通过偏振态控制阵列板时被分割成许多子光束,每一子光束的振幅和位相均受到不同程度的调制。故,当激光通过光场偏振态控制阵列板后转化为目标光场,也可以实现完全的非偏振光,该光束经聚焦透镜汇聚到靶面,焦斑光强中由于子光束干涉所带来的斑纹能够消除,从而能实现靶面的均匀辐照。 The technical solution of the present invention is: there is an optical field polarization state control array plate in the system device, the plate plays the role of polarization control, and is composed of p×q processing units, and each unit is equipped with a controllable electro-optic crystal, such as KDP crystals. By adding an appropriate voltage, the electro-optic crystal plate produces a suitable phase delay for the two components of the incident polarized light, so that the outgoing light becomes the polarized light we need, and the purpose of modulating the polarization state of the incident beam is achieved. When the laser passes through the polarization control array plate, it is divided into many sub-beams, and the amplitude and phase of each sub-beam are modulated to different degrees. Therefore, when the laser passes through the light field polarization state control array plate and then transforms into the target light field, it can also achieve complete unpolarized light. The speckle can be eliminated, so that the uniform irradiation of the target surface can be realized.
本发明同现有的偏振控制技术相比,其优点在于可以通过控制各单元晶片所加电压来实现对入射的任意场分布光场的各子光束的偏振态进行有效控制,进而将其转换为预期的偏振状态。例如,可以将任意光场转化为非偏振光。系统装置中的主要部件是光场偏振态控制阵列板,易于制作,结构简单。 Compared with the existing polarization control technology, the present invention has the advantage that the polarization state of each sub-beam of the incident arbitrary field distribution light field can be effectively controlled by controlling the voltage applied to each unit chip, and then converted into expected polarization state. For example, arbitrary light fields can be converted to unpolarized light. The main component in the system device is the optical field polarization state control array plate, which is easy to manufacture and simple in structure.
附图说明 Description of drawings
下面结合附图和实施例对本发明进一步说明。 The present invention will be further described below in conjunction with the accompanying drawings and embodiments.
图1是本发明的装置示意图。 Figure 1 is a schematic diagram of the device of the present invention.
图2是光场偏振态控制阵列板的示意图。 Fig. 2 is a schematic diagram of an optical field polarization state control array plate.
图3是光场偏振态控制阵列板的第一个实施例的示意图。 Fig. 3 is a schematic diagram of a first embodiment of an optical field polarization state control array plate.
图4是光场偏振态控制阵列板的第二个实施例的示意图。 Fig. 4 is a schematic diagram of a second embodiment of an optical field polarization control array plate.
图1中1位相调制器,2光栅,3光场偏振态控制阵列板,4聚焦透镜,5接收光场的靶面 In Figure 1, 1 phase modulator, 2 gratings, 3 light field polarization state control array plate, 4 focusing lens, 5 target surface for receiving light field
图2中的光场偏振态控制阵列板是一个p×q的可控旋光晶体阵列。 The optical field polarization control array plate in Fig. 2 is a p×q controllable optical rotation crystal array.
图3中的光场偏振态控制阵列板是一个随机偏振板。 The optical field polarization state control array plate in Fig. 3 is a random polarizing plate.
图4中的光场偏振态控制阵列板是一个正交偏振板。 The optical field polarization control array plate in Fig. 4 is a crossed polarizer.
具体实施方案 specific implementation plan
本发明的实施例一,光场偏振态控制阵列板是一个随机偏振板,如图3所示。经过位相调制的光场通过光栅后发生色散,经过随机偏振板后分成多个子光束,且各自的偏振态发生随机的改变,最后经透镜聚焦在靶面上。利用随机偏振板,通过改变每个子单元光束的偏振态,从而在大孔径光束内部产生偏振态各异的子光束。 In Embodiment 1 of the present invention, the optical field polarization control array plate is a random polarizing plate, as shown in FIG. 3 . The phase-modulated light field undergoes dispersion after passing through the grating, and is divided into multiple sub-beams after passing through a random polarizing plate, and their respective polarization states change randomly, and finally focus on the target surface through the lens. A random polarizing plate is used to generate sub-beams with different polarization states inside the large-aperture beam by changing the polarization state of each sub-unit beam.
激光束经本系统传输时,光谱色散匀滑技术中的频谱展宽和光栅色散,使得各频率的子光束产生的干涉散斑在色散方向上产生位移,从而在时间平均尺度上实现了对焦斑的匀滑。而偏振态控制阵列板的使用对焦斑场分布的主要影响在于对不同波长在x、y方向叠加的振幅调制和位相不同,使得输出光在不同波长处的偏振态不同,导致光束偏振态发生明显的变化,实现了消偏振。 When the laser beam is transmitted through the system, the spectrum broadening and grating dispersion in the spectral dispersion smoothing technology make the interference speckle generated by the sub-beams of each frequency shift in the direction of dispersion, thus realizing the focus spot on the time average scale smooth. The main effect of the use of the polarization state control array plate on the field distribution of the focal spot is that the amplitude modulation and phase of different wavelengths superimposed in the x and y directions are different, so that the polarization states of the output light at different wavelengths are different, resulting in a significant change in the polarization state of the beam The change achieves depolarization.
本发明的实施方案二,光场偏振态控制阵列板是一个正交偏振板,如图4所示。对于正交偏振板,则使各个子单元的出射光束只能是某一偏振方向的线偏光。 Embodiment 2 of the present invention, the optical field polarization control array plate is an orthogonal polarizing plate, as shown in FIG. 4 . For the crossed polarizing plates, the outgoing light beams of each subunit can only be linearly polarized light in a certain polarization direction.
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Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN107402454A (en) * | 2017-08-31 | 2017-11-28 | 东南大学 | The non-linear ellipse inclined rotating device of radial variations is realized based on elliptical polarization vectorial field |
CN113091896A (en) * | 2021-03-18 | 2021-07-09 | 西北工业大学 | Method and light path for dynamically measuring complete information of any light field based on polarization grating |
Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN101546050A (en) * | 2009-05-05 | 2009-09-30 | 中国科学院上海光学精密机械研究所 | Electronically controlled phase-shift crystal birefringence free-space optical bridge |
CN102253493A (en) * | 2011-06-27 | 2011-11-23 | 广东工业大学 | Laser beam uniform radiation optical system |
-
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Patent Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN101546050A (en) * | 2009-05-05 | 2009-09-30 | 中国科学院上海光学精密机械研究所 | Electronically controlled phase-shift crystal birefringence free-space optical bridge |
CN102253493A (en) * | 2011-06-27 | 2011-11-23 | 广东工业大学 | Laser beam uniform radiation optical system |
Non-Patent Citations (3)
Title |
---|
K. TSUBAKIMOTO, T. JITSUNO, N. MIYANAGA, M. NAKATSUKA, T. KANABE: "Suppression of speckle contrast by using polarization property on second harmonic generation", 《OPTICS COMMUNICATIONS》, vol. 103, no. 34, 15 November 1993 (1993-11-15) * |
江秀娟: "高功率激光驱动器光束匀滑技术的研究进展", 《激光与光电子学进展》, vol. 47, no. 9, 30 September 2010 (2010-09-30) * |
肖峻,吕百达: "偏振控制板对干涉斑纹的匀滑特性", 《中国激光》, vol. 27, no. 7, 31 July 2000 (2000-07-31) * |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN107402454A (en) * | 2017-08-31 | 2017-11-28 | 东南大学 | The non-linear ellipse inclined rotating device of radial variations is realized based on elliptical polarization vectorial field |
CN113091896A (en) * | 2021-03-18 | 2021-07-09 | 西北工业大学 | Method and light path for dynamically measuring complete information of any light field based on polarization grating |
CN113091896B (en) * | 2021-03-18 | 2023-03-14 | 西北工业大学 | Method and light path for dynamically measuring complete information of any light field based on polarization grating |
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