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1.
We show that bright-dark vector solitons are possible in biased two-photon photorefractive crystals under steady-state conditions. The analytical solutions of these vector solitons can be obtained if the intensities of the two vector components are approximately equal. When the intensities of the two vector components differ, the vector soliton pair solutions can be determined using simple numerical integration procedures. The stability of the bright-dark vector solitons has been investigated numerically.  相似文献   

2.
A group of additional invariance (polarization symmetry) of the Prock equations is considered, whose generators satisfy the algebra SU (3) (massive field) of SU (2) (massless field). The investigative method developed in the paper is directly related to the physical content of the transformations of the symmetry being discussed: the change in the polarization field. The small Lorentz group is a sub-group of the transformations being discussed. Possible physical applications of polarization symmetry are discussed.Translated from Izvestiya Vysshikh Uchebnykh Zavedenii, Fizika, Ho. 7, pp. 77–80, July, 1982.  相似文献   

3.
We calculate bisoliton solutions by using a slowly varying stroboscopic equation. The system is characterized in terms of a single dimensionless parameter. We find two branches of solutions and describe the structure of the tails for the lower-branch solutions.  相似文献   

4.
We investigate the focusing property and the polarization evolution characteristics of hybridly polarized vector fields in the focal region. Three types of hybridly polarized vector fields, namely azimuthal-variant hybridly polarized vector field, radial-variant hybridly polarized vector field, and spatial-variant hybridly polarized vector field, are experimentally generated. The intensity distributions and the polarization evolution of these hybridly polarized vector fields focused under low numerical aperture (NA) are experimentally studied and good agreements with the numerical simulations are obtained. The three-dimensional (3D) state of polarization and the field distribution within the focal volume of these hybridly polarized vector fields under high-NA focusing are studied numerically. The optical curl force on Rayleigh particles induced by tightly focused hybridly polarized vector fields, which results in the orbital motion of trapped particles, is analyzed. Simulation results demonstrate that polarization-only modulation provided by the hybridly polarized vector field allows one to control both the intensity distribution and 3D elliptical polarization in the focal region, which may find interesting applications in particle trapping, manipulation, and orientation analysis.  相似文献   

5.
It has been shown that the principally new-type solitons and bisolitons are generated during the pulse impact of ultrasound and hypersound on crystal monatomic materials in addition to the known solitons. New-type bisolitons analogous to the bisolitons previously found by an analytical approach have been discovered with the use of the molecular dynamics method. It has been shown that the dispersion curve of these bisolitons is close to the dispersion curve of the conventional solitons. A subsonic compression soliton, the dispersion curve of which crosses the phonon dispersion curve, has been found along with the known supersonic compression soliton. The characteristics of the new-type solitons and bisolitons in uranium and plutonium crystal lattices are presented.  相似文献   

6.
We experimentally observe polarization-locked vector solitons in optical fiber. Polarization locked-vector solitons use nonlinearity to preserve their polarization state despite the presence of birefringence. To achieve conditions where the delicate balance between nonlinearity and birefringence can survive, we studied the polarization evolution of the pulses circulating in a laser constructed entirely of optical fiber. We observe two distinct states with fixed polarization. This first state occurs for very small values birefringence and is elliptically polarized. We measure the relative phase between orthogonal components along the two principal axes to be +/-pi/2. The relative amplitude varies linearly with the magnitude of the birefringence. This state is a polarization locked vector soliton. The second, linearly polarized, state occurs for larger values of birefringence. The second state is due to the fast axis instability. We provide complete characterization of these states, and present a physical explanation of both of these states and the stability of the polarization locked vector solitons. (c) 2000 American Institute of Physics.  相似文献   

7.
王思聪  李向平 《中国光学》2016,9(2):185-202
作为光波最重要的本征物理属性之一,光场偏振态在研究光与物质相互作用中占有重要地位。矢量光场的波前调控为其聚焦场提供了更加复杂、更加灵活可控的振幅、相位以及偏振态分布,丰富了光与物质相互作用的手段,为材料表征提供了传统线偏振、圆偏振光场所不可替代的研究方法,具有重要的物理意义和实际应用价值。本文将综述矢量光场最新的研究进展,详细介绍矢量光场的偏振态特性、产生方法,以及紧聚焦轴对称矢量光场波前调控在远场小尺度光斑的产生、磁光记录、单分子/颗粒取向探测、任意三维偏振态的产生、高密度数据存储、信息加密以及矢量光场波前重构等方面的重要应用。  相似文献   

8.
Liuzhan Pan  Baida Lü   《Optik》2002,113(10):459-463
Based on Wolf's general tensorial theory of coherence, in which the vector nature of electromagnetic fields is considered, the closed-form propagation equation of vector Gaussian-Schell-model (GSM) beams passing through a paraxial optical ABCD system is derived, which shows the general applicable advantage, and is used to study polarization changes of GSM beams in passage through a thin lens. It is found that polarization changes are dependent on the propagation distance, focal length of the lens, beam and coherence parameters and bandwidth of the source spectrum in general. A comparison with the previous results is also made.  相似文献   

9.
Liuzhan Pan  Baida Lü   《Optik》2002,113(9):459-463
Based on Wolf's general tensorial theory of coherence, in which the vector nature of electromagnetic fields is considered, the closed-form propagation equation of vector Gaussian-Schell-model (GSM) beams passing through a paraxial optical ABCD system is derived, which shows the general applicable advantage, and is used to study polarization changes of GSM beams in passage through a thin lens. It is found that polarization changes are dependent on the propagation distance, focal length of the lens, beam and coherence parameters and bandwidth of the source spectrum in general. A comparison with the previous results is also made.  相似文献   

10.
双光子光折变介质中非相干耦合亮-暗屏蔽光伏孤子对   总被引:1,自引:1,他引:0  
对有外加电场的双光子光伏光折变晶体中两束偏振方向和波长都相同的互不相干光束的耦合进行研究,给出产生亮-暗双光子光折变屏蔽光伏孤子对需满足的条件.以Cu:KNSBN晶体作为研究对象,选取α=117.3,β=83.79,η=1.5×10-4,σ=104,δ=0.005,r=10时,给出双光子光折变晶体中的非相干耦合亮-暗屏蔽光伏孤子对2个孤子分量光强的空间分布,证明有外加电场的双光子光伏光折变晶体中存在非相干耦合亮-暗屏蔽光伏孤子对,指出孤子对是由偏振态和波长都相同的两束互不相干光形成的,当外加电场方向和晶体中光伏电场的方向与晶体光轴方向相同时,双光子光折变晶体中可支持亮孤子峰值光强稍大于暗孤子最大光强的非相干耦合亮-暗孤子对,当外加电场方向和晶体中光伏电场的方向与晶体光轴方向相反时,双光子光折变晶体中可支持亮孤子峰值光强稍小于暗孤子最大光强的非相干耦合亮-暗孤子对.  相似文献   

11.
The coupling of two mutually incoherent optical beams with the same polarization and wavelength in two-photon photovoltaic photorefractive crystal is studied, it is predicted theoretically that incoherently coupled bright-dark photovoltaic spatial soliton pairs are possible due to two-photon photorefractive effect. The existing conditions of these soliton pairs in the crystal are discussed in detail. The intensity profile of these soliton pairs is shown by numerical calculation under the parameters of relevant crystal.  相似文献   

12.
The cross section and density matrix elements fore + e ?V+X ande + e ?B+X are calculated in the γ-Z 0 interference region. The Feynman-Field model for the quark fragmentation functions is extended to include baryons and spin of the particles. Possibilities for obtaining more specific information about the spin dependence of the fragmentation mechanism and the weak coupling of quarks are discussed.  相似文献   

13.
We demonstrate the emission of bright pulse and dark pulse in a simple all-fiber ring cavity laser by using self-pulsing technique. The switching between bright pulse and dark pulse can be realized by properly rotating the polarization controller (PC). Meanwhile, the bright-dark pulse can also be generated in the fiber laser and is experimentally verified to be on two different orthogonal polarization axis of the cavity fiber. Our experimental results show that the bright pulse, the dark pulse or the bright-dark pulse can be obtained in an all-fiber laser by using self-pulsing technique.  相似文献   

14.
It has been shown using the molecular dynamics method that new-type solitons and bisolitons are generated under the action of pulsed of ultrasound and hypersound on the crystalline single-atom materials. The dispersion curve of new-type bisolitons adjoins the dispersion curve of conventional solitons. A subsonic compression soliton is found, the dispersion curve of which intersects the phonon dispersion curve. Nuclei of new phases are generated under the inelastic collision of solitons in the fcc and hcp crystal systems at the early stage of structural phase transitions. The solitons of the new undulator type, which generate nuclei, are found. Characteristics of solitons and bisolitons in crystal lattices of uranium and plutonium are presented.  相似文献   

15.
温度对双光子独立明-暗空间屏蔽孤子对稳定性的影响   总被引:2,自引:2,他引:0  
在忽略损耗和扩散的情况下,采用数值方法研究温度对串联双光子光折变晶体回路中独立明-暗屏蔽孤子对演化和稳定性的影响.结果表明:在给定温度下晶体回路中形成稳态明-暗孤子对,当一个晶体的温度改变且温度变化不大时,另一块晶体中支持的孤子将转变为另一个稳态孤子;当温度变化过大时,这个孤子将变得不稳或发生周期性的压缩或膨胀甚至崩溃.在独立屏蔽空间孤子对中,暗孤子对温度的敏感程度比明孤子强.  相似文献   

16.
 根据光波耦合方程及亮-暗孤子对解,对稳态情况下多束互不相干的光束在有外加电场的双光子非光伏光折变晶体中的传播进行分析,给出产生亮-暗双光子光折变屏蔽光伏孤子族需满足的条件。证明有外加电场双光子非光伏光折变晶体中存在非相干耦合亮-暗混合屏蔽孤子族,孤子族由偏振态和波长都相同的多束互不相干的光形成。当外加电场方向和晶体光轴方向相同时,双光子光折变晶体可支持亮孤子族总峰值光强稍大于暗孤子族总峰值光强的的非相干耦合亮-暗混合孤子族,当外加电场方向与晶体光轴方向相反时,双光子光折变晶体可支持亮孤子族总峰值光强稍小于暗孤子族总峰值光强的非相干耦合亮-暗混合孤子族。  相似文献   

17.
《中国物理 B》2021,30(5):54205-054205
We experimentally demonstrated a stable multi-wavelength bright–dark pulse pair in a mode-locked thulium-doped fiber laser(TDFL). The nonlinear polarization rotation(NPR) and nonlinear optical loop mirror(NOLM) were employed in a figure-eight cavity to allow for multi-wavelength mode-locking operation. By incorporating different lengths of high birefringence polarization-maintaining fiber(PMF), the fiber laser could operate stably in a multi-wavelength emission state. Compared with the absence of the PMF, the birefringence effect caused by PMF resulted in rich multi-wavelength optical spectra and better intensity symmetry and stability of the bright–dark pulse pair.  相似文献   

18.
用极化晶体谱仪探测X射线极化度   总被引:1,自引:1,他引:0  
为了研究等离子体各向异性及确定高温等离子体中电子束的存在,研制了X射线极化晶体谱仪,探讨了极化光谱学的理论,推演了X射线极化度的计算方法.谱仪能够在两个相互垂直的方向分别对X射线进行探测,垂直方向晶体分析器使用云母球面晶体,水平方向为PET平面晶体,摄谱元件采用成像板.在激光聚变研究中心2×10 J激光装置上进行了摄谱实验.实验结果表明,PET晶体分光效果理想,获得了铝的类He共振线(w)、磁四级M2跃迁x线、互组合跃迁y线以及禁戒谱线z线,适合于研究X射线极化光谱学;云母晶体得到铝的类He共振线,其伴线光谱不明显.分析了谱仪垂直方向信号微弱的原因,提出了改进极化晶体谱仪的方案.  相似文献   

19.
为了研究等离子体各向异性及确定高温等离子体中电子束的存在,研制了X射线极化晶体谱仪,探讨了极化光谱学的理论,推演了X射线极化度的计算方法.谱仪能够在两个相互垂直的方向分别对X射线进行探测,垂直方向晶体分析器使用云母球面晶体,水平方向为PET平面晶体,摄谱元件采用成像板.在激光聚变研究中心2×10 J激光装置上进行了摄谱实验.实验结果表明,PET晶体分光效果理想,获得了铝的类He共振线(w)、磁四级M2跃迁x线、互组合跃迁y线以及禁戒谱线z线,适合于研究X射线极化光谱学;云母晶体得到铝的类He共振线,其伴线光谱不明显.分析了谱仪垂直方向信号微弱的原因,提出了改进极化晶体谱仪的方案.  相似文献   

20.
基于亚波长偏振光栅的偏振光分束器设计   总被引:3,自引:2,他引:1  
利用琼斯矩阵和矢量傅里叶系数方法分析了二元亚波长偏振光栅的偏振特性和衍射效率,并给出了相应的数学解析式.研究发现,通过入射光的偏振可以控制不同衍射输出级的偏振态,且0级输入偏振态与输出偏振态始终相同,而其它级次除线偏光外都与入射偏振态相反.当二元亚波长偏振光栅的位相延迟分别设置为0.62π和π时,可以将二元亚波长偏振光栅设计为1→3或1→2的偏振光分束器,且分束器具有衍射效率高、宽带宽、对入射角的变化不甚敏感的特点.  相似文献   

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