椭圆高斯光束的分数傅里叶变换

利用分数傅里叶变换与Wigner分布函数旋转等效的性质 ,推导出了椭圆高斯光束在分数傅里叶变换平面上的光强分布和束宽的解析公式。研究了椭圆高斯光束光强和束宽随分数傅里叶变换阶数变化的规律 ,并给出了数值计算结果     

分数傅里叶变换面上厄米-拉盖尔-高斯光束的变换特性

为了研究厄米-拉盖尔-高斯(HLG)光束在分数傅里叶变换(FRFT)面上的变换特性,利用柯林斯(Collins)公式,导出了其通过分数傅里叶变换系统后,在分数傅里叶变换面上的光强分布解析式.并利用此解析式作数值计算,研究了其在分数傅里叶变换面上的光强分布特性.研究表明,厄米-拉盖尔-高斯光束在分数傅里叶变换面上的光强分布受参量α,模指数m,n和分数傅里叶变换阶数p的影响.光强分布随p和α周期性变化,周期分别为2,2π.此外,厄米-拉盖尔-高斯光束通过分数傅里叶变换系统后,光束形状保持不变.     

Bessel-Gaussian光束在分数傅里叶变换面上的光强分布

利用广义衍射积分方法,研究了Bessel-Gaussian(BG)光束的分数傅里叶变换特性,推导出了BG光束通过分数傅里叶变换光学系统后,光场分布的解析公式,利用该公式对BG光束经分数傅里叶变换后光强的分布规律进行了数值分析。研究结果表明,分数傅里叶变换阶数p对BG光束的光强分布有明显影响,光强分布随分数傅里叶变换阶数p呈周期性变化。     

厄米-双曲余弦-高斯光束通过对称化光学系统的变换

研究了用于厄米高斯光束对称化的光学系统对像散厄米双曲余弦高斯光束的变换。分析了偏心参数和模阶数对变换后的厄米双曲余弦高斯光束对称性的影响,通过大量数值计算说明复杂像散厄米双曲余弦高斯光束对称化的物理意义。     

像散透镜对双曲余弦-高斯光束参量的影响

为了进一步研究双曲余弦-高斯光束的特性,从广义惠更斯-菲涅耳衍射积分公式出发,对双曲余弦-高斯光束通过像散透镜后的光束参量,例如束宽和远场发散角的相对误差作了研究.结果表明,束宽和远场发散角的相对误差与像散因子C2,偏心参量α,瑞利长度z0以及透镜焦距f等有关.几何焦面上x和y方向束宽的相对误差与像散系数C2和偏心参量α变化相同,而在像方束腰处两方向相对误差变化迥异.此外,束宽的相对误差还与传输距离z有关.因像散影响,在x和y方向远场发散角一般不相等,并且还与偏心参量α有关.     

双曲余弦-高斯光束的相干模分解

利用傅里叶变换和正交模系展开法,推导出了双曲余弦—晶斯光束的M2因子和归一化模系数的解析表达式,从而建立了双曲余弦-高斯光束的相干模分解理论。提出了一种在实验室中产生双曲余弦-高斯光束的简单方法。     

部分相干cosh-Gaussian光束通过大气湍流后的聚焦特性

为了研究部分相干双曲余弦高斯光束通过大气湍流中传输后的聚焦特性,采用了ABCD矩阵光学的方法进行分析研究,取得了光强分布、束腰半径以及桶中功率的解析式,并用于描述部分相干双曲余弦高斯光束通过大气湍流的聚焦特性。结果表明,在不同湍流强度下,部分相干双曲余弦高斯光束和双曲余弦高斯光束在经过大气湍流后有不同的聚焦特性;使用桶中功率和束腰半径作为评价参量,大气湍流对完全相干双曲余弦高斯的影响更严重;大气湍流对聚焦部分相干双曲余弦高斯光束的影响要大于准直光束。该结果对部分相干光束聚焦特性的研究有一定的理论指导意义,对合成光束傍轴聚焦系统的设计有工程指导意义。     

非傍轴部分相干厄米-余弦-高斯光束传输特性

为了研究非傍轴部分相干厄米-余弦-高斯光束传输特性,运用Wigner分布函数法,从空间域和频率域对非傍轴部分相干厄米-余弦-高斯光束传输特性进行了理论分析,得出了该光束1阶情况下在空间、频率域系统的解析传输公式及光强分布表达式,分析了这些表达式中3个主要参量f,fσ和g对厄米-余弦-高斯光束在自由空间传输的影响。结果表明,在调制参量g不变时,束腰参量f和相干参量fσ对非傍轴部分相干厄米-余弦-高斯光束的非傍轴性起了至关重要的作用;非傍轴部分相干厄米-余弦-高斯光束在传输过程中随着g的改变,不能保持其光强分布形状,有前移趋势。     

非傍轴部分相干厄米-余弦-高斯光束传输特性

为了研究非傍轴部分相干厄米-余弦-高斯光束传输特性,运用Wigner分布函数法,从空间域和频率域对非傍轴部分相干厄米-余弦-高斯光束传输特性进行了理论分析,得出了该光束1阶情况下在空间、频率域系统的解析传输公式及光强分布表达式,分析了这些表达式中3个主要参量f,fσ和g对厄米-余弦-高斯光束在自由空间传输的影响。结果表明,在调制参量g不变时,束腰参量f和相干参量fσ对非傍轴部分相干厄米-余弦-高斯光束的非傍轴性起了至关重要的作用;非傍轴部分相干厄米-余弦-高斯光束在传输过程中随着g的改变,不能保持其光强分布形状,有前移趋势。     

余弦平方-高斯光束通过像散透镜的焦开关

为了研究余弦平方.高斯光束通过像散透镜后的焦开关现象,应用Collins公式推导出了聚焦余弦平方-高斯光束轴上光强分布的表达式,通过数值运算得到了像散参量对轴上光强分布的影响.结果表明,在给定光束参量和光束菲涅耳数的条件下,光束入射面位置不同时,余弦平方-高斯光束通过像散透镜后的相对焦移随像散参量变化而变化,确定了在此...     

Fractional Fourier transform for annular flat-topped beams

The fractional Fourier transform (FRFT) is applied to treat the propagation of annular flat-topped beams. Based on the definition of FRFT in the cylindrical coordinate system, analytical formulae are derived for annular flat-topped beams through the FRFT optical systems. By using the formulae, the properties of annular flat-topped beams in the FRFT plane are illustrated numerically. The results show that the intensity distribution properties in the FRFT plane are closely related to the fractiona...     

Propagation properties of beams generated by Gaussian mirror resonator in fractional Fourier transform plane

Based on the definition of the fractional Fourier transform (FRFT) and irradiance moments in the cylindrical coordinate system, the propagation expressions and kurtosis parameter of beams generated by Gaussian mirror resonator passing through the ideal fractional Fourier transformation systems are obtained. The propaga-tion properties and kurtosis parametric characteristic of the beams in the FRFT plane are analyzed in detail. Some numerical examples are given to illustrate the analytical results. The influences of the fractional order on the intensity distribution and the kurtosis parameter of the beams are also investigated. The results show that the intensity distribution and the kurtosis parameter of the beams in the FRFT plane are closely related to the fractional order and beam parameters.     

非傍轴截断双曲余弦高斯光束的M2因子

基于功率密度的二阶矩方法,对非傍轴截断双曲余弦高斯(ChG)光束的束宽、远场发散角和M2因子进行了研究.数值计算结果表明,非傍轴截断ChG光束的M2因子不仅与截断参数δ、偏心参数α有关,而且与初始束腰宽度和波长之比w0/λ有关.在δ足够小时,M2因子可小于1.当δ→ 0时,远场发散角趋于渐近值63.435°.对于α=0(Ω0=0)和δ→∞的特例,我们的结果分别退化为非傍轴截断高斯光束和非傍轴无截断ChG光束的M2因子.     

一种基于分数阶Fourier变换的雷达运动目标检测算法

针对雷达回波为多分量LFM信号时,时频分析存在的交叉项干扰问题,提出了一种基于分数阶Fourier变换(Fractional Fourier Transform,FRFT)的伪Wigner分布(PWD).该方法通过在参数平面按阈值进行峰值搜索确定变换域阶次,再在相应的分数阶Fourier域计算PWD,有效地抑制了交叉项的干扰,有利于更好地提取信号的时频信息.仿真实验证明了在强背景噪声下该算法的有效性.     

分数阶傅里叶变换在雷达多目标检测和参数估计中的应用

介绍了分数阶傅里叶变换的基本原理和基本性质。结合时域和频域上扫频滤波器的原理推导出了分数域上的扫频滤波器的实现形式。利用分数阶傅里叶变换对线性调频信号有很好的聚焦性的性质,提出了基于分数阶傅里叶变换的雷达多目标检测和参数估计算法。解决了在强度相差较大的强分量信号中检测和估计弱分量LFM信号参数的问题。仿真结果表明了该算法的有效性。     

Closed-form discrete fractional and affine Fourier transforms

The discrete fractional Fourier transform (DFRFT) is the generalization of discrete Fourier transform. Many types of DFRFT have been derived and are useful for signal processing applications. We introduce a new type of DFRFT, which are unitary, reversible, and flexible; in addition, the closed-form analytic expression can be obtained. It works in performance similar to the continuous fractional Fourier transform (FRFT) and can be efficiently calculated by the FFT. Since the continuous FRFT can be generalized into the continuous affine Fourier transform (AFT) (the so-called canonical transform), we also extend the DFRFT into the discrete affine Fourier transform (DAFT). We derive two types of the DFRFT and DAFT. Type 1 is similar to the continuous FRFT and AFT and can be used for computing the continuous FRFT and AFT. Type 2 is the improved form of type 1 and can be used for other applications of digital signal processing. Meanwhile, many important properties continuous FRFT and AFT are kept in the closed-form DFRFT and DAFT, and some applications, such as filter design and pattern recognition, are also discussed. The closed-form DFRFT we introduce has the lowest complexity among all current DFRFTs that is still similar to the continuous FRFT     

Relations between fractional operations and time-frequencydistributions, and their applications

The fractional Fourier transform (FRFT) is a useful tool for signal processing. It is the generalization of the Fourier transform. Many fractional operations, such as fractional convolution, fractional correlation, and the fractional Hilbert transform, are defined from it. In fact, the FRFT can be further generalized into the linear canonical transform (LCT), and we can also use the LCT to define several canonical operations. In this paper, we discuss the relations between the operations described above and some important time-frequency distributions (TFDs), such as the Wigner distribution function (WDF), the ambiguity function (AF), the signal correlation function, and the spectrum correlation function. First, we systematically review the previous works in brief. Then, some new relations are derived and listed in tables. Then, we use these relations to analyze the applications of the FRPT/LCT to fractional/canonical filter design, fractional/canonical Hilbert transform, beam shaping, and then we analyze the phase-amplitude problems of the FRFT/LCT. For phase-amplitude problems, we find, as with the original Fourier transform, that in most cases, the phase is more important than the amplitude for the FRFT/LCT. We also use the WDF to explain why fractional/canonical convolution can be used for space-variant pattern recognition     

高斯光束通过空间滤波器的传输特性

采用矩阵分解和用有限个复高斯函数之和逼近硬边光阑窗口函数相结合的方法,从柯林斯衍射积分公式出发,对高斯光束通过空间滤波器的传输特性进行了分析,得到了相应的解析式。通过对解析式的数值模拟,得出了直观的结果,并进行了误差分析。数值计算结果表明,最佳滤波小孔尺寸的选择和计算误差均与光束的截断参数有关。在此基础上,进一步研究了空间滤波器具有像传递功能时,高斯光束和平顶高斯光束(N=12)通过空间滤波器的传输特性,得出了截断参数与滤波后光强分布的关系,并证实了此方法也可用于计算其他类型光束通过空间滤波器的传输。     

部分相干双曲正弦-高斯光束的传输和聚焦特性

为了研究部分相干双曲正弦-高斯(SHG)光束通过像散透镜的传输和聚焦特性,利用部分相干光的传输公式,推导了光束通过像散透镜后光强分布解析的表达式,并据此得到了光束束腰宽度、远场发散角和M2因子的解析表达式,并对光束强度分布和束腰宽度进行了数值计算和分析。结果表明:部分相干ShG光束聚焦的光强分布与像散系数C6,空间相干参数,离心参数a,菲涅耳数Nw和位置(x,y,z)有关。像散导致x和y方向束宽不同。但M2因子与像散无关,并随相干性的增加和离心参数的减小而减小。适当改变像散和空间相干性,在几何焦面和其它位置可实现部分相干ShG光束的空间整形。