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非傍轴贝塞尔-高斯光束在自由空间的传输 总被引:2,自引:2,他引:0
从瑞利-索末菲衍射积分出发,推导出任意阶非傍轴贝塞尔-高斯光束在自由空间传输的解析表达式.非傍轴贝塞尔光束和非傍轴高斯光束等的传输方程都可以作为本文一般结果的特例而得出.物理分析和数值计算表明,当高斯和贝塞尔部分的横向尺度与波长相比拟或小于波长时,应当用非傍轴方法处理. 相似文献
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矢量非傍轴双曲余弦-高斯光束 总被引:3,自引:3,他引:0
引入了矢量非傍轴双曲余弦-高斯(ChG)光束概念。使用矢量瑞利-索末菲衍射积分公式推导出了矢量非傍轴ChG光束在自由空间传输的解析公式。矢量非傍轴ChG光束轴上和远场的解析式以及傍轴结果作为一般传输公式的特例给出。研究表明,对矢量非傍轴ChG光束,其非傍轴性主要由f参数决定,但偏心参数会影响其横向光强剖面形状和非傍轴行为。 相似文献
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运用非傍轴光束传输的矢量矩理论,对非傍轴矢量高斯光束的传输特性进行了系统的研究.结果表明,基于二阶矩定义的横向光束宽度在光束传播过程中满足简单的双曲线变化规律,并且给出了光束传输因子的解析表达式.就高度非傍轴情形,进一步给出了简洁的计算公式,在高斯光源线度趋向零的极限情形下,横向的最大发散角为90°.同时,还推广到了傍轴情形,得到了与原有傍轴公式稍有区别的结果,而且光束传输因子始终保持略大于1最后,对非傍轴矢量高斯光束和非傍轴标量高斯光束的传输进行了比较,结果显示对于线度在两个波长范围之内的高斯光源发散
关键词:
矢量高斯光束
光束传输
非傍轴
二阶矩 相似文献
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文章提出一种横向激发的任意线偏振高斯光束,该光束场量的模与传统的任意线偏振高斯光束具有相同的模,在源场区,其满足自由空间无源场的场方程。同时利用瑞利—索末菲衍射积分对该高斯光束的非傍轴传输特性进行了解析研究,给出了空间光强分布、束腰和远场发散角的解析通式,发现该类光束的远场光强呈一平顶空心光束。 相似文献
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基于矢量瑞利-索末菲衍射积分公式,得出了波动方程的一个解,它代表矢量非傍轴离轴高斯光束,其在自由空间的传输方程表示为解析的结果.矢量非傍轴离轴高斯光束的轴上和远场公式,矢量非傍轴高斯光束的传输方程,以及傍轴的结果都可作为一般表达式的特例而得出.研究表明,f参数对光束的非傍轴特性有重要影响,而离心参数也影响非傍轴行为.与共轴情况不同的是,对离轴情况,在y方向存在场的纵向分量.
关键词:
激光光学
矢量非傍轴离轴高斯光束
瑞利-索末菲衍射积分
f参数
离轴参数 相似文献
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矢量可控空心光束的非傍轴传输 总被引:1,自引:1,他引:0
提出了矢量可控空心光束概念,可控空心光束可以很好地描写中心光强不完全为零的圆对称窄心光束,具有可用多个参最米控制中央暗斑尺寸、形式简单易于分析、其传输变换特性更接近于实际等特点.利用矢量瑞利-索末菲衍射积分公式,导出了矢量可控空心光束的非傍轴传输解析公式,从所得结果可退化得到傍轴近似结果.利用导出的公式计算分析了矢量可控空心光束在自由空间的非傍轴传输特性,并与傍轴结果进行了比较分析.结果表明矢量可控空心光束在近场很好地保持其空心光场分布特性;参量f和传输距离决定了矢量可控空心光束的非傍轴特性. 相似文献
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《Optics Communications》2003,220(4-6):401-412
We used generalised Lorenz–Mie scattering theory (GLMT) to compare submicron-sized particle optical trapping in a single focused beam and a standing wave. We focus especially on the study of maximal axial trapping force, minimal laser power necessary for confinement, axial trap position, and axial trap stiffness in dependency on trapped sphere radius, refractive index, and Gaussian beam waist size. In the single beam trap (SBT), the range of refractive indices which enable stable trapping depends strongly on the beam waist size (it grows with decreasing waist). On the contrary to the SBT, there are certain sphere sizes (non-trapping radii) that disable sphere confinement in standing wave trap (SWT) for arbitrary value of refractive index. For other sphere radii we show that the SWT enables confinement of high refractive index particle in wider laser beams and provides axial trap stiffness and maximal axial trapping force at least by two orders and one order bigger than in SBT, respectively. 相似文献
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By using a small number of Gaussian basis functions, one can synthesize the wave fields radiated from planar and focused piston transducers in the form of a superposition of Gaussian beams. Since Gaussian beams can be transmitted through complex geometries and media, such multi-Gaussian beam models have become powerful simulation tools. In previous studies the basis function expansion coefficients of multi-Gaussian beam models have been obtained by both spatial domain and k-space domain methods. Here, we will give an overview of these two methods and relate their expansion coefficients. We will demonstrate that the expansion coefficients that have been optimized for circular piston transducers can also be used to generate improved field simulations for rectangular probes. It will also be shown that because Gaussian beams are only approximate (paraxial) solutions to the wave equation, a multi-Gaussian beam model is ultimately limited in the accuracy it can obtain in the very near field. 相似文献
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On the basis of superposition of beams, a group of virtual sources that generate a cosh-Gaussian wave is identified. A closed-form expression is derived for this cosh-Gaussian wave, which, in the appropriate limit, yields the paraxial approximation for the cosh-Gaussian beam. From this expression, the paraxial approximation and the nonparaxial corrections of all orders for the corresponding paraxial cosh-Gaussian beam are determined. 相似文献
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Marston PL 《The Journal of the Acoustical Society of America》2011,129(4):1773-1782
A superposition of zero-order Bessel beams is examined that closely resembles an idealized paraxial Gaussian beam, provided the superposition is not tightly focused. Plots compare wavefield properties in the focal region and in the far field for different values of kw(0), the product of the wavenumber k, and the focal-spot-radius w(0). The superposition (which is an exact solution of the Helmholtz equation) has the important property that the scattering by an isotropic sphere can be calculated without any approximations for the commonly considered case of linear waves propagating in an inviscid fluid. The nth partial wave amplitude is similar to the case of plane-wave illumination except for a weighting factor that depends on incomplete gamma functions. An approximation for the weighting factor is also discussed based on a generalization of the Van de Hulst localization principle for a sphere of radius a at the focus of a Gaussian beam. Examples display differences between the directionality of the scattering with the plane wave case even though for the cases displayed, ka does not exceed 2 and w(0)∕a is not less than 2. Properties of tightly focused wavefields and the partial wave weighting factors are discussed. 相似文献
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A family of closed-form expressions for the scalar field of strongly focused Gaussian beams in oblate spheroidal coordinates is given. The solutions satisfy the wave equation and are free from singularities. The lowest-order solution in the far field closely matches the energy density produced by a sine-condition, high-aperture lens illuminated by a paraxial Gaussian beam. At the large waist limit the solution reduces to the paraxial Gaussian beam form. The solution is equivalent to the spherical wave of a combined complex point source and sink but has the advantage of being more directly interpretatable. 相似文献
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Power Density Distribution Simulation and Relevant Heat Effect Calculation of a High-power CO_2 Laser with Low Order Modes 总被引:3,自引:0,他引:3
1 Introduction Intheindustrialapplicationresearchoflaserbeamheatprocessingandtreatment,duetotheshortinteractiontimeoflaserwiththematerial,theheat affectedareaislimitedintheareanearthe positionirradiatedbythelaserbeam .Supposedthattheworkpieceisasemi inf… 相似文献
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Gil Ariel Björn Engquist Nicolay M. Tanushev Richard Tsai 《Journal of computational physics》2011,230(6):2303-2321
A new numerical method for approximating highly oscillatory wave fields as a superposition of Gaussian beams is presented. The method estimates the number of beams and their parameters automatically. This is achieved by an expectation–maximization algorithm that fits real, positive Gaussians to the energy of the highly oscillatory wave fields and its Fourier transform. Beam parameters are further refined by an optimization procedure that minimizes the difference between the Gaussian beam superposition and the highly oscillatory wave field in the energy norm. 相似文献
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Starting from the vectorial Rayleigh diffraction integral formula and without using the far-field approximation, a solution of the wave equation beyond the paraxial approximation is found, which represents vectorial non-paraxial elliptical Gaussian beams in free space. The far-field expressions for non-paraxial Gaussian beams and elliptical Gaussian beams can be regarded as special cases treated in this paper. Some basic propagation properties of vectorial non-paraxial elliptical Gaussian beams, including the irradiance distribution, phase term, beam widths and divergence angles are studied. Numerical results are given and illustrated. 相似文献
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The analytical expression for the beam propagation factor (M2-factor) of Gaussian Schell-model (GSM) array beams propagating through atmospheric turbulence is derived. It is shown that the M2-factor of GSM array beams depends on the beam number, the relative beam separation distance, the beam coherence parameter, the type of beam superposition, and the strength of turbulence. The turbulence results in an increase of the M2-factor. However, for the superposition of the intensity the M2-factor is less sensitive to turbulence than that for the superposition of the cross-spectral density function. The M2-factor of GSM array beams is larger than that of the corresponding Gaussian array beams. However, the M2-factor of GSM array beams is less affected by turbulence than that of the corresponding Gaussian array beams. For the superposition of the cross-spectral density function a minimum of the M2-factor of GSM array beams may appear in turbulence, which is even smaller than that of the corresponding single GSM beams. 相似文献