Skip to content
DraconiticResearch
Search Sources API
197,768 studies31 sourcesUpdated 10 min ago
PreprintCC BY 4.0arXiv

Fermionic Unruh effect revisited: Entanglement and correlation dynamics under symmetric transformations

Abstract

A uniformly accelerated observer perceives the Minkowski vacuum as a thermal bath, so acceleration acts as a noise channel on correlations shared with an inertial partner. For a Dirac field in the standard treatment, the resulting map is a one-sided amplitude-damping channel, and entanglement and quantum discord survive at infinite acceleration. We introduce a symmetric Unruh-like map in which the vacuum and the one-particle state both exchange amplitude with the inaccessible Rindler region; for a Bell state it yields a bit-flip channel whose flip probability is the Fermi-Dirac occupation at the Unruh temperature. Using negativity, mutual information, and all six pairwise quantum discords, we find that the entanglement and discord between the inertial observer and the accessible mode vanish together at infinite acceleration, leaving only one bit of classical correlation. These results show that the fate of quantum correlations in noninertial frames depends on the structure of the Minkowski-Rindler map.

Related

  1. Symmetry-driven correlation patterns in one-dimensional periodic fermionic systems: closed-form expressions and exact selection rules for correlation functions, entanglement entropies and mutual information
    Celestino Angeli
    arXivPreprintCC BY-NC-ND 4.0Full textQuantum physics & quantum informationarXiv
  2. Fermionic Genuine Multiparty Entanglement
    James Allen, Liuke Lyu, William Witczak-Krempa
    arXivPreprintCC BY 4.0Full textCondensed matterQuantum physics & quantum informationarXiv
  3. Operator-Space Entanglement Entropy in Random Fermionic Gaussian Dynamics
    Pablo Bayona-Pena, Elena Gramellini, Lorenzo Piroli
    arXivPreprintarXiv licenceFull textMathematical physicsQuantum physics & quantum informationarXiv
  4. Diagrammatic Monte Carlo for Fermionic Rényi Entanglement Entropy
    Boyuan Shi
    arXivPreprintarXiv licenceFull textComputational physicsCondensed matterarXiv
  5. Vectorized Symmetric and Fermionic Tensor Network Implementations for GPU-Accelerated Variational Monte Carlo
    Si-Jing Du, Johnnie Gray, Ao Chen +1
    arXivPreprintarXiv licenceFull textComputational physicsCondensed matterarXiv
BibTeX
@misc{monem2026fermionic,
  title = {{Fermionic Unruh effect revisited: Entanglement and correlation dynamics under symmetric transformations}},
  author = {Omid Yahyayi Monem and Hosein Mohammadzadeh},
  howpublished = {arXiv},
  year = {2026},
  month = oct,
  doi = {10.48550/arxiv.2610.38387},
  eprint = {2610.38387},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2610.38387},
  note = {CC BY 4.0},
}
RIS
TY  - UNPB
TI  - Fermionic Unruh effect revisited: Entanglement and correlation dynamics under symmetric transformations
AU  - Omid Yahyayi Monem
AU  - Hosein Mohammadzadeh
PY  - 2026
DA  - 2026/10/28
PB  - arXiv
DO  - 10.48550/arxiv.2610.38387
UR  - https://arxiv.org/abs/2610.38387
AB  - A uniformly accelerated observer perceives the Minkowski vacuum as a thermal bath, so acceleration acts as a noise channel on correlations shared with an inertial partner. For a Dirac field in the standard treatment, the resulting map is a one-sided amplitude-damping channel, and entanglement and quantum discord survive at infinite acceleration. We introduce a symmetric Unruh-like map in which the vacuum and the one-particle state both exchange amplitude with the inaccessible Rindler region; for a Bell state it yields a bit-flip channel whose flip probability is the Fermi-Dirac occupation at the Unruh temperature. Using negativity, mutual information, and all six pairwise quantum discords, we find that the entanglement and discord between the inertial observer and the accessible mode vanish together at infinite acceleration, leaving only one bit of classical correlation. These results show that the fate of quantum correlations in noninertial frames depends on the structure of the Minkowski-Rindler map.
ER  -