2021
DOI: 10.1088/2040-8986/abedf6
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Transformation of asymmetric Schell-model beams with a wavefront-folding interferometer

Abstract: We consider a class of random light beams, which are generated by inserting an asymmetric Schell-model beam into a wavefront-folding interferometer. Typical propagation behavior of such optical beams modulated by several legitimate complex coherence states has been investigated. In certain cases, these beams exhibit novel rotationally symmetric intensity patterns with rectangular or lattice-like lobes, and the pattern and location of each lobe can be controlled by adjusting the source coherence parameters. Bes… Show more

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Cited by 2 publications
(3 citation statements)
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“…On substituting equation ( 25) first into equation ( 29) and then into equation (28), we could obtain the CSDM elements in the far field. Taking r 1 = r 2 = r, the far-field spectral density has the form…”
Section: Transformation Of Partially Polarized Schell-model Beamsmentioning
confidence: 99%
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“…On substituting equation ( 25) first into equation ( 29) and then into equation (28), we could obtain the CSDM elements in the far field. Taking r 1 = r 2 = r, the far-field spectral density has the form…”
Section: Transformation Of Partially Polarized Schell-model Beamsmentioning
confidence: 99%
“…The CSDM of the field in the far zone could be directly determined by substituting equation ( 33) into equations ( 29) and (28). Then the far-field spectral density and the DOP along the x direction take the forms…”
Section: Transformation Of Radially Polarized Gsm Beamsmentioning
confidence: 99%
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