2016
DOI: 10.1364/ol.41.003181
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Beyond the diffraction limit via optical amplification

Abstract: In a previous article we suggested a method to overcome the diffraction limit behind a telescope. We refer to theory and recent numerical simulations, and test whether it is indeed possible to use photon amplification to enhance the angular resolution of a telescope or a microscope beyond the diffraction limit. An essential addition is the proposal to select events with above-average ratio of stimulated to spontaneous photons. We find that the diffraction limit of a telescope is surpassed by a factor ten for a… Show more

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Cited by 19 publications
(13 citation statements)
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“…There are so many other superresolution ideas that going through them all would not be feasible. We list here only a few more: superoscillation [123], amplification [124], and postselection [125]. They either require steep trade-offs with the SNR or have questionable statistics [126,127].…”
Section: F Superoscillation Amplification Postselectionmentioning
confidence: 99%
“…There are so many other superresolution ideas that going through them all would not be feasible. We list here only a few more: superoscillation [123], amplification [124], and postselection [125]. They either require steep trade-offs with the SNR or have questionable statistics [126,127].…”
Section: F Superoscillation Amplification Postselectionmentioning
confidence: 99%
“…communication). Additionally, as we discuss below, QT cannot be placed in the plane conjugated to the pupil, that is -QT cannot be implemented as a small device located after the mirror, as proposed by Kellerer & Ribak (2016). The basic theory of quantum physics and optics indicate that the position of a photon, whose wevefunction is reduced to the size of telescope's aperture, cannot be retrieved with the accuracy exceeding the diffraction limit.…”
Section: Modelmentioning
confidence: 99%
“…As for the practical implementation of probabilistic single-photon amplification to astronomical imaging: in previous publications we have considered the possibility to send the incoming astronomical photon through a medium of excited atoms and to use stimulated emission as the amplification mechanism. 11,12 The noise then takes the form of spontaneous emissions. As mentioned here in introduction, an amplifier adds an average of g noise photons per amplified mode (see for example 6).…”
Section: Probabilistic Amplification In the Context Of Astronomical Imentioning
confidence: 99%