1999
DOI: 10.1103/physrevlett.83.1938
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Noiseless Optical Amplification of Images

Abstract: We used a spatially broadband optical parametric amplifier for image amplification. In the phasesensitive configuration of the amplifier, we observed noiseless amplification of input images. For a gain of Ӎ2.5, we measured noise-figure values of (0.2 6 0.6) and (0.4 6 0.5) dB, respectively, for two amplifiers of different lengths. These experimental values agree with theory (for an ideal noiseless amplifier the noise figure is 0 dB) and are almost 2 dB lower than the quantum limit of an ideal phaseinsensitive … Show more

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Cited by 130 publications
(60 citation statements)
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“…The difference between PSA and PIA gain reaches the theoretical limit of ~ 6dB at the input pump power of 33 dBm, as indicated in Fig. 2(b) [30].…”
Section: Theoretical Modelmentioning
confidence: 79%
“…The difference between PSA and PIA gain reaches the theoretical limit of ~ 6dB at the input pump power of 33 dBm, as indicated in Fig. 2(b) [30].…”
Section: Theoretical Modelmentioning
confidence: 79%
“…This process may therefore be utilized in distributed multi-wavelength imaging or image processing, where objects are placed in the path of one or more of these fields of different wavelengths and the intensities or cross-correlations are measured. Two examples of phenomena based on three-wave mixing, optical parametric oscillation (OPO) and optical parametric amplification (OPA), have been studied extensively and many interesting phenomena of spatial correlation [11], pattern formation [12,13], and reduced-noise image amplification [14,15] have been reported.…”
Section: Introductionmentioning
confidence: 99%
“…In recent years, there has been an increasing interest in the field of quantum imaging, in which nonclassical states of light are used as light sources [1,2,3,4,5,6,7,8,9,10,11,12]. Special attentions are focused on entangled-photon coincidence imaging [1,2,3,4,5,6,7,8].…”
mentioning
confidence: 99%