Transfer of entanglement from nonlocal photon to non-Gaussian CV states

• URL: http://arxiv.org/abs/2509.17700v1
• Date: Mon, 22 Sep 2025 12:35:33 GMT
• Title: Transfer of entanglement from nonlocal photon to non-Gaussian CV states
• Authors: Mikhail S. Podoshvedov, Sergey A. Podoshvedov,
• Abstract summary: We propose the mechanism of transfer of quantum entanglement from a nonlocal photon to two initially separate single-mode squeezed vacuum states.<n>We estimate the probability of transfer of maximum entanglement at sufficiently high brightness to be 0.2344.<n>Such a perfect TQE from the nonlocal photon to a maximally parity-entangled CV state can be considered the most suitable for applications.
• Score: 0.0
• License: http://creativecommons.org/licenses/by/4.0/
• Abstract: Continuous variable (CV) entanglement refers to the type of entanglement of quantum wave-like systems that are described by continuous variables in an inherently infinite-dimensional space. It can become a crucial resource for quantum communication, sensing and computation. We propose the mechanism of transfer of quantum entanglement (TQE) from a nonlocal photon to two initially separate single-mode squeezed vacuum (SMSV) states. The nonlocal photon is the only original quantum resource from which entanglement is transferred to CV states of a certain parity without them directly interacting with each other in a deterministic manner. Measurement induced CV parity entanglement is tuned using initial squeezing and the beam splitter (BS) parameter allowing us to estimate the probability of transfer of maximum entanglement at sufficiently high brightness to be 0.2344 . If, instead of the original SMSV states, we use those from which one photon is initially subtracted, then the heralded technique can turn the probabilistic maximum entanglement transfer protocol into a nearly deterministic one, the probability of which is >0.98. Such a perfect TQE from the nonlocal photon to a maximally parity-entangled CV state can be considered the most suitable for applications, since it preserves the trade-off between the probability and brightness of the output non-Gaussian states.

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