2019
DOI: 10.1088/1367-2630/ab4afb
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Quantum tomography of light states by photon-number-resolving detectors

Abstract: We address state reconstruction by photon-number-resolving detectors, and demonstrate that they may be effectively exploited to perform quantum tomography of states of light. In particular, we find that the pattern function technique, originally developed for optical homodyne tomography, may be also applied to discrete data. Our results open new perspectives for quantum-state reconstruction in the mesoscopic regime, and pave the way to the use of photon-number-resolving-based detection schemes in Quantum Infor… Show more

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Cited by 20 publications
(11 citation statements)
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References 51 publications
(60 reference statements)
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“…In Ref. [18], we have demonstrated that the probability distribution for the photon-number difference can be written in terms of the joint photon-number statistics q(m, n) measured at the two BS outputs:…”
Section: Methodsmentioning
confidence: 99%
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“…In Ref. [18], we have demonstrated that the probability distribution for the photon-number difference can be written in terms of the joint photon-number statistics q(m, n) measured at the two BS outputs:…”
Section: Methodsmentioning
confidence: 99%
“…The results obtained in Ref. [18] suggest that the intensity of the LO must be increased not only when the energy of the reconstructed states increases, but also when the states exhibit peculiar Wigner functions with, for instance, many oscillations in the phase space. In this last scenario, increasing the LO intensity allows a better sampling of the corresponding "discretized" homodyne probability distributions and, thus, a more faithful tomographic reconstruction.…”
Section: Introductionmentioning
confidence: 96%
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“…Through this analysis, we also study the limits imposed by nonlinearities and saturation effects of some parts of the acquisition chain, having in mind the exploitation of the high dynamic range of SiPMs to detect well-populated states of light. Indeed, reliably detecting the number of photons in every pulse of highly-populated states is the key resource to implement homodyne-like schemes with a mesoscopic local oscillator (up to 50 mean photon numbers), as required to achieve an optimal quantum state reconstruction [8,9]. Increasing the dynamic range is also required if the considered states of light are characterized by large fluctuations, such as in the case of superthermal states of light [10,11].…”
Section: Introductionmentioning
confidence: 99%