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Irradiance variance for convergent Gaussian beams using nondimensional beam parameters

机译:使用非潜能光束参数的收敛高斯光束的辐照方差

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The longitudinal and radial irradiance variance for a convergent Gaussian beam is examined in terms of two pairs of nondimensional beam parameters, the first pair approximately ega $EQ $lambda@L/$pi@W$-o$/$+2$/ and approximately ega$-o$/ $EQ 1 $MIN L/R$-o$/ associated with the beam when transmitted, and the second pair given by $Lambda $EQ $lambda@L/$pi@W$+2$/ and $Theta $EQ 1 $PLU L/R associated with the received beam. Here, $lambda is wavelength, L is path length, R$-o$/ and R are radii of curvature of the phase front at the transmitter and receiver, respectively, and W$-o$/ and W are the beam radii at the transmitter and receiver. With the addition of $lambda and L, either of these beam parameter pairs completely characterizes the diffractive propagation environment for a lowest-order paraxial Gaussian beam, and is fundamental in the analytic expression of the irradiance variance. Special attention is paid to differences between the perfectly focused beam and the nearly focused beam. We also show that every beam has a convergent counterpart with identical diffractive irradiance behavior at the receiver, but decreased irradiance variance.
机译:在两对非潜能光束参数方面检查了会聚高斯光束的纵向和径向辐照方差,第一对大约是EGA $ eq $ llambda @ l / $ pi @ w $ -o $ / $ + 2 $ /大约是ega $ -o $ / $ eq 1 $ min l / r $ -o $ /与光束传输时,第二对给出$ lambda $ eq $ lambda @ l / $ pi @ w $ + 2 $ /和$ theta $ eq 1 $ plu l / r与接收的光束相关联。在这里,$ lambda是波长,l是路径长度,R $ -o $ /和r分别是发射器和接收器的相位前正面曲率的半径,而W $ -o $ /和w是光束半径发射器和接收器。随着$ Lambda和L的添加,这些光束参数对中的任何一个都完全表征了最低阶段高斯梁的衍射传播环境,并且是辐照方差的分析表达的基础。特别关注完美聚焦光束和近乎聚焦光束之间的差异。我们还表明,每个光束在接收器处具有具有相同衍射辐照度行为的收敛对应物,但辐照方差降低。

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