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Anatoly S. Chirkin

Publications and source records attributed to Anatoly S. Chirkin.

2 recordsLinked to original sources

Existence Criterion of Solutions to the Inverse Problem of Photocount Statistics Obtained by the Inverse Bernoulli Transform

It is shown that the applicability conditions for the inverse Bernoulli transform method for solving the inverse problem of photocount statistics are determined by the fulfillment of the associativity condition for multiplying the matrices included in this transformation. A general criterion for evaluating the photocount distributions $Q_{m}$ in the case of few-photon light, which makes it possible to establish whether the solution to the inverse problem of photocount statistics by inverse Bernoulli transform method is applicable for $η<0.5$, is found. As an example of application of the obtained criterion, the critical quantum efficiency $η_{cr}$ is found for compound Poisson distribution, below which the solution of the inverse problem of photocount statistics becomes incorrect. Additionally it is shown that the normalization of $Q_{m}$ is not sufficient to obtain a correct solution using the inverse Bernoulli transform.

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Correlations of multiplexed quantum ghost images and improvement of the quality of restored image

The currently used ghost image schemes traditionally involve two-mode entangled light states or incoherent radiation. Here, application of four-mode entangled light states is considered. It is shown that multiplexed ghost images (MGI) formed by four-mode entangled quantum light states have mutual spatial correlations determined by the 8th order field correlation functions. A special algorithm to calculate high-order correlations of Bose operators was developed. We also demonstrate that the accounting of MGI correlations allows us to improve the quality of the restored image of an object when processing MGI by measurement reduction method. Computer modelling of recovery of the image from MGI was carried out. It is established that in the considered example the signal-to-noise ratio of the reduced ghost image is $4.6$ times higher than the best signal-to-noise ratio for the ghost images themselves.

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