Generalized beam-propagation factor of partially coherent beams propagating through hard-edged apertures

2002 ◽  
Vol 19 (7) ◽  
pp. 1370 ◽  
Author(s):  
Bin Zhang ◽  
Xiaoliang Chu ◽  
Qiang Li
2011 ◽  
Vol 321 ◽  
pp. 256-260
Author(s):  
Bang Yuan Hao

For partially coherent hollow Gaussian beam (HGB), the turbulent distance, in which all of the spatial and angular spreading and the beam propagation factor increasing due to turbulence can be neglected, has been investigated in detail. It is shown that the turbulent distance of partial coherent HGBs increases with increasing beam order and wavelength, and decreasing turbulent parameter and coherent parameter. With increasing waist width, the turbulent distance first increases and then decreases. Furthermore, the turbulent distance of a HGB is much larger than that of the corresponding Gaussian Schell-model (GSM) beam when choosing the appropriate value of the waist width, implying that a HGB may be more appropriate to be used in optical communication links than a GSM beam.


Optik ◽  
2014 ◽  
Vol 125 (13) ◽  
pp. 3166-3171 ◽  
Author(s):  
Yingshun Wang ◽  
Jie Lian ◽  
Shang Gao ◽  
Xiao Wang ◽  
Zhaozong Sun ◽  
...  

2011 ◽  
Vol 43 (7) ◽  
pp. 1225-1228 ◽  
Author(s):  
Guohua Wu ◽  
Tonggang Zhao ◽  
Jianhua Ren ◽  
Junyi Zhang ◽  
Xiaolei Zhang ◽  
...  

Photonics ◽  
2021 ◽  
Vol 8 (2) ◽  
pp. 60
Author(s):  
Milo W. Hyde

In this paper, we present a method to independently control the field and irradiance statistics of a partially coherent beam. Prior techniques focus on generating optical field realizations whose ensemble-averaged autocorrelation matches a specified second-order field moment known as the cross-spectral density (CSD) function. Since optical field realizations are assumed to obey Gaussian statistics, these methods do not consider the irradiance moments, as they, by the Gaussian moment theorem, are completely determined by the field’s first and second moments. Our work, by including control over the irradiance statistics (in addition to the CSD function), expands existing synthesis approaches and allows for the design, modeling, and simulation of new partially coherent beams, whose underlying field realizations are not Gaussian distributed. We start with our model for a random optical field realization and then derive expressions relating the ensemble moments of our fields to those of the desired partially coherent beam. We describe in detail how to generate random optical field realizations with the proper statistics. We lastly generate two example partially coherent beams using our method and compare the simulated field and irradiance moments theory to validate our technique.


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