2004
DOI: 10.1140/epjd/e2003-00323-2
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Direct experimental characterization of the Bose-Einstein distribution of spatial fluctuations of spontaneous parametric down-conversion

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2005
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Cited by 24 publications
(27 citation statements)
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“…(Accurate measurements of the photon statistics in the high gain regime of PDC are described e.g. in [23].) According to definition (8), it follows therefore that the excess noise coincides with the mean number of photons per mode:…”
Section: Fragility Of Quantum Correlation Toward Imperfect Detectionmentioning
confidence: 99%
“…(Accurate measurements of the photon statistics in the high gain regime of PDC are described e.g. in [23].) According to definition (8), it follows therefore that the excess noise coincides with the mean number of photons per mode:…”
Section: Fragility Of Quantum Correlation Toward Imperfect Detectionmentioning
confidence: 99%
“…In the condition of the experiment the pump duration is slightly longer than the PDC coherence time while the pixel area is smaller than the coherence area, so that M is expected to be only slightly larger than unity [31]. Using this, (5) becomes…”
Section: Detection Of Quantum Spatial Correlation: Spatial Analogmentioning
confidence: 99%
“…The width of the coherence area in the far field, 0.07 mrad (FWHM), is proportional to the inverse of the width of this beam [19] and is much smaller than the 0.32-mrad lateral size of the CCD pixel. Moreover, the mean number of photons for one spatiotemporal mode is less than 10 −2 , resulting in theoretical Bose-Einstein photon distribution [20] that is undistinguishable from a Poisson distribution. Indeed, the number of amplified temporal modes is approximately 40 [19] and the number of amplified spatial modes on a pixel is on the order of (0.32/0.07) 2 20.…”
Section: Measurement Of Sub-shot-noise Correlations Between Pixelsmentioning
confidence: 99%