Quantum ghost polarimetry with entangled photons

Sergey Magnitskiy; Dmitriy Agapov; Anatoly Chirkin

doi:10.1364/OL.450206

Optics Letters
Vol. 47,
Issue 4,
pp. 754-757
(2022)
•https://doi.org/10.1364/OL.450206

Quantum ghost polarimetry with entangled photons

Sergey Magnitskiy, Dmitriy Agapov, and Anatoly Chirkin

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Sergey Magnitskiy, Dmitriy Agapov, and Anatoly Chirkin, "Quantum ghost polarimetry with entangled photons," Opt. Lett. 47, 754-757 (2022)

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- Quantum Optics and Quantum Communication
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About this Article
History
- Original Manuscript: December 2, 2021
- Revised Manuscript: December 23, 2021
- Manuscript Accepted: December 24, 2021
- Published: February 2, 2022

Abstract

The theory of the formation of polarization ghost images in biphoton light of spontaneous parametric scattering is developed. On the basis of the developed theory, the quantum ghost polarimetry concept has been suggested, which makes it possible to obtain two-dimensional maps of the polarization properties of objects by measuring a set of correlation functions obtained in various polarization states of photons. For objects with linear dichroism, a complete set of measurement states is found, which allows for obtaining the maps of the distributions of absorption, value, and azimuth of anisotropy.

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Data underlying the results presented in this paper are not publicly available at this time but may be obtained from the authors upon reasonable request.

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Number of Measurement Configuration, $k$	Polarization State after Controller	Normalized Correlation Function $g (r)$
1	$\| H ⟩$	$g_{1} (r) = T (r) [1 - (1 - P^{2} (r) 1) \sin^{2} θ (r)]$
2	$\| V ⟩$	$g_{2} (r) = T (r) [1 - (1 - P^{2} (r)) \cos^{2} θ (r)]$
3	$\frac{\| H ⟩ + \| V ⟩}{\sqrt{2}}$	$g_{3} (r) = \frac{T (r)}{2} [1 + P^{2} (r) + (1 - P^{2} (r)) \sin 2 θ (r)]$

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