2008
DOI: 10.1080/09500340802169553
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Determination of the coherency matrix of a broadband stochastic electromagnetic light beam

Abstract: The statistical ensemble of a fluctuating, statistically-stationary electromagnetic light beam is presented in terms of a 2 Â 2 matrix, so-called coherency matrix. The method to determine such matrix for a quasi-monochromatic light beam has been proposed for many years. In this paper, we demonstrate that the method needs to be only slightly modified to determine the matrix elements of a broadband stochastic electromagnetic light beam, if one uses the representation of statistical wave fields in the space-frequ… Show more

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Cited by 15 publications
(3 citation statements)
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“…The polarization state for the FP beam with polar angle Θ = π/3, π/2, and 2π/3 is located in the northern part, on the equator, and in the southern part of the higher-order Poincaré sphere, respectively. The Stokes parameters for the partially coherent beam are measured with the standard method [44].…”
Section: Resultsmentioning
confidence: 99%
“…The polarization state for the FP beam with polar angle Θ = π/3, π/2, and 2π/3 is located in the northern part, on the equator, and in the southern part of the higher-order Poincaré sphere, respectively. The Stokes parameters for the partially coherent beam are measured with the standard method [44].…”
Section: Resultsmentioning
confidence: 99%
“…Based on the parameter measurement system of EGSM beams proposed in [8], the experimental measurement of the received beam radius σ xyout can be carried out easily and efficiently. Moreover, according to [61], by using the polarizer and quarter-wave plate, we can also measure the degree of polarization in the receiver plane P out (0, z, ω).…”
Section: Degree Of the Polarizationmentioning
confidence: 99%
“…This wavelength region is known as the optical window of biological samples since water absorption and blood absorption is minimum caused it becomes transparent [6,7]. Without contacting the sample, OCT focuses the near-infrared light beam deep below the biological sample's surface and gates the back-reflection light through the low-temporal coherence [8,9] of the incident light in order to section depth information of the sample at microns resolution. The low coherence gating can be achieved by the use of Michelson interferometer [10] or Mach-Zehnder interferometer [11,12].…”
Section: Introductionmentioning
confidence: 99%