Distribution de la Somme des Photoélectrons Détectés en L Points sous Eclairement Gaussien Partiellement Cohérent

1971 ◽  
Vol 49 (24) ◽  
pp. 3064-3074 ◽  
Author(s):  
Jacques Bures ◽  
Claude Delisle ◽  
Andrzej Zardecki

The analysis of the photocount distribution in incoherent Gaussian light detected in L space points of a photodetector is extended to the case of partially coherent light. The second moment of the derived distribution is exact. A function η is introduced which accounts for the spatial coherence aspect of light as does the function ξ, (Mandel) for the temporal coherence aspect. A more general function ζ, which for cross-spectrally pure light reduces to the product ζ = ηξ, depends on both spatial and temporal characteristics of coherence. It is shown both theoretically and experimentally that many different geometrical configurations yield the same normalized second moment. A pseudo-thermal source [Formula: see text] where T is the detection time and Tc the coherence time) is used for the experimental verification.

1972 ◽  
Vol 50 (8) ◽  
pp. 760-768 ◽  
Author(s):  
Jacques Bures ◽  
Claude Delisle ◽  
Andrzej Zardecki

The theoretical distribution, with exact second moment, of the number of photoelectrons emitted by an extended photodetector illuminated with partially coherent light is first derived. Then the parameter N, the number of degrees of freedom, is obtained from the second moment of the distribution, for [Formula: see text] (T is the detection time and Tc the coherence time). N is then plotted as a function of the surface of the detector expressed in three different ways for both circular source and detector and square source and detector. In both cases the source is considered to be of uniform brightness. An elementary surface called the surface of coherence is determined by extrapolating towards small values the asymptotical behavior of N for large values of the detection surface. For both sources, this surface of coherence is equal to [Formula: see text]. λ0 is the mean wavelength, D the distance between the source and the detector, and Ss the surface of the source.


1991 ◽  
Vol 131 ◽  
pp. 10-14
Author(s):  
Daniel F.V. James

The interferometric mapping of astronomical objects relies on the van-Cittert Zernike theorem, one of the major results of the theory of partially coherent light [see, Bom and Wolf (1980), chapter 10]. This theorem states that the degree of spatial coherence of the field from a distant spatially incoherent source is proportional to the Fourier transform of the intensity distribution across the source. Measurement of the degree of spatial coherence, by, for example, measuring the visibility of interference fringes, allows the object to be mapped by making an inverse Fourier transform. (For a full description of this technique see Thompson, Moran and Swenson, 1986.)In this paper I present a summary of the results an investigation into what happens when the distant source is not spatially coherent (James, 1990). Using a heuristic model of a spherically symmetric partially coherent source, an analytic expression for the error in the measurement of the effective radius, expressed as a function of coherence area, can be obtained.


2021 ◽  
Vol 51 (2) ◽  
Author(s):  
Yushuang Wang ◽  
Xuanxuan Ji ◽  
Ziyang Chen ◽  
Jixiong Pu

We develop a Q-switched degenerate laser, delivering a partially coherent light pulse of duration about 16 ns. The spatial coherence of the output laser pulse can be varied by tuning the spatial filter inside the laser resonator, and the oscillating transverse mode structure can be determined by measuring the degree of coherence of the output laser pulse. It is shown that the larger is the diameter of the spatial filter, the more are the oscillating transverse modes, and the lower is the degree of coherence. Based on coherent-mode representation for the partially coherent source, we can estimate the transverse mode contribution to the output partially coherent laser. The experimental results on suppressing speckle demonstrate that the generated partially coherent light possesses the characteristics of rapid reduction of spatial coherence, making it an ideal source for high-speed imaging and ranging applications.


2018 ◽  
Vol 26 (3) ◽  
pp. 2928 ◽  
Author(s):  
J. Alejandro Gonzaga-Galeana ◽  
Jorge R. Zurita-Sánchez

1979 ◽  
Vol 129 (9) ◽  
pp. 151
Author(s):  
G.S. Egorov ◽  
S.N. Mensov ◽  
Nikolai S. Stepanov

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