2017
DOI: 10.1063/1.4994669
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Synthesis of non-uniformly correlated partially coherent sources using a deformable mirror

Abstract: The near real-time synthesis of a non-uniformly correlated partially coherent source using a low-actuator-count deformable mirror is demonstrated. The statistical optics theory underpinning the synthesis method is reviewed. The experimental results of a non-uniformly correlated source are presented and compared to theoretical predictions. A discussion on how deformable mirror characteristics such as actuator count and pitch affect source generation is also included.

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Cited by 39 publications
(12 citation statements)
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“…In both cases, the physical meaning of the above expansion is that a partially coherent source can be thought of as the superposition of a set of mutually uncorrelated, perfectly coherent, and suitably weighted fields. Of course, this also represents a way to physically synthesize partially coherent source [19,22,23,26,40,63], especially when they are not of the Schell-model type [6,44,45]. The superposition usually involves an infinite number of coherent fields but for practical applications a finite number is often enough for a good representation of the CSD function [27,44].…”
Section: Synthesismentioning
confidence: 99%
See 1 more Smart Citation
“…In both cases, the physical meaning of the above expansion is that a partially coherent source can be thought of as the superposition of a set of mutually uncorrelated, perfectly coherent, and suitably weighted fields. Of course, this also represents a way to physically synthesize partially coherent source [19,22,23,26,40,63], especially when they are not of the Schell-model type [6,44,45]. The superposition usually involves an infinite number of coherent fields but for practical applications a finite number is often enough for a good representation of the CSD function [27,44].…”
Section: Synthesismentioning
confidence: 99%
“…Among them, Gaussian Schell-model (GSM) sources, where both the spectral degree of coherence and the irradiance profile are Gaussianly shaped [1,24], have been extensively studied and characterized [25][26][27][28][29][30][31][32]. Since the publication of the superposition rule [33,34], that have eased the design of physically realizable CSD's, different kind of sources, of the Schell-model type [20,21,35,36] or not [6,[37][38][39][40][41][42][43][44][45] have been proposed.…”
Section: Introductionmentioning
confidence: 99%
“…These SLM characteristics and their effects on beam control have been discussed before (please see Refs. [26,45,58,59,61] for more information). The MATLAB R version R2018b scripts (.m files) are included as Supplementary Materials to this paper.…”
Section: Resultsmentioning
confidence: 99%
“…The second method starts with a coherent, polarized source, and then transforms the vector components of that source into realizations drawn from the ensemble of all optical fields consistent with the desired electromagnetic PCS [5,14,26,37,[44][45][46][47][48][49][50]. The transformation from coherent, polarized source to stochastic field realization is accomplished using spatial light modulators (SLMs).…”
Section: Introductionmentioning
confidence: 99%
“…In addition, several methods have been proposed to experimentally generate the prescribed DOC of a PCB, for example by using a spatial light modulator, intra-cavity modulation and a deformable mirror, etc. [24][25][26][27]. However, the aforementioned studies are confined to PCBs whose initial intensity distributions have a Gaussian function.…”
Section: Introductionmentioning
confidence: 99%