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- W2156876136 abstract "It is well known that totally incoherent light cannot exhibit first-order with photons that are uncorrelated,i.e., the normalized first-order correlation function is g(1)(0) = 0, whereas the second-order correlationfunction is g(2)(0) = 1. Less familiar is the fact that both chaotic and coherent sources can exhibit first-order interference,so that merely using the term interference is ambiguous. If fact, some previous QIQC presentationshave centered around whether or not two-photon correlations are actually a form of two-photon interference.1Another area of ambiguity concerns the detection of quantum state coherence using interference.2 In an attemptto disambiguate the concept of interference, we examine associated photon states using chaotic sources and theHanbury Brown and Twiss (HBT) detection of bunched photons. The unambiguous determination of coherentquantum states has important applications for:(1) Atomic Bose-Einstein condensate (BEC) determined using scattered laser interference3(2) Exciton-Polariton BEC determined using emitted photon interference4(3) Coherent light states.(4) Characterizing photon statistics.(5) Characterization of extended sources.In this paper, we present imaging results for topics 3-5. The difficulties of HBT data acquisition are generallyunderappreciated. An advantage of our approach is super-linear speedup through the development of a newimaging device consisting of a 2-dimensional array of single-photon avalanche detectors.5, 6 A 4 × 4 arrayenables 120 HBT coincidence experiments to be run in parallel to generate the 2-dimensional distribution ofg(2)(x) spatial correlations, thus making plausible the term g2 camera for this quantum imaging device." @default.
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- W2156876136 date "2008-08-28" @default.
- W2156876136 modified "2023-09-27" @default.
- W2156876136 title "Experiments supporting the concept of a g(2)-camera" @default.
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- W2156876136 doi "https://doi.org/10.1117/12.795166" @default.
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