Skip to content
DraconiticResearch
Search Sources API
203,234 studies31 sourcesUpdated 1 h ago
PreprintarXiv licencearXiv

Non-Hermiticity of an anomalous superradiant phase

Abstract

We present a Hermitian squeezing-Dicke model as a minimal closed-system setting for non-Hermitian many-body physics. Squeezing generates an effective parity-time (𝒫𝒯) symmetry and exchanges gainy and lossy eigenmodes without dissipation. We identify an anomalous dynamical superradiant phase (DSRP) that exhibits by a mean-field superradiant order in the 𝒫𝒯 symmetry-breaking regime, accompanied by a β„€2-symmetry-breaking ground-state quantum phase transition. Additionally, it undergoes a 𝒫𝒯-breaking dynamical phase transition at an exceptional point (EP). The excitation energy vanishes near both boundaries, giving critical slowing down. The vacuum photon number is divergent at the ground-state transition but is finite and nonanalytic at the EP, distinguishing the DSRP from the conventional superradiant phase and from a standard dynamical instability. Squeezing causes the coupling phase to act as an artificial magnetic flux, which yields flux-controlled nonreciprocal quantum amplification in the DSRP. Our results offer an alternative pathway to non-Hermitian many-body physics and nonreciprocal quantum amplification in closed Hermitian systems.

Related

  1. Anomalous superradiant phases in a quantum Rabi zigzag chain under a synthetic gauge field
    Jun-Bo Tang, Lin-Jun Li, Bin Wei +1
    arXivPreprintarXiv licenceFull textQuantum physics & quantum informationarXiv
  2. Extensively degenerate superradiant phase in a giant-atom quantum Rabi ring
    Shu He, Li-Wei Duan
    arXivPreprintarXiv licenceFull textQuantum physics & quantum informationarXiv
  3. Global Phase Locking in Superradiant Chorus Emissions
    Xin Tao, Fulvio Zonca, Liu Chen
    arXivPreprintCC BY-NC-ND 4.0Full textPlasma physicsarXiv
  4. Anomalous temperature dependence in phase transitions via ballistic coalescence
    Nalina Vadakkayil, Sutapa Roy, Jiarul Midya +1
    arXivPreprintCC BY 4.0Full textCondensed matterarXiv
  5. Anomalous Structures of Fisher Zero Lines in Biorthogonal Dynamical Quantum Phase Transitions
    Wen-Hui Nie, Chong Li, Lin-Cheng Wang
    arXivPreprintarXiv licenceFull textQuantum physics & quantum informationarXiv
BibTeX
@misc{lu2026nonhermiticity,
  title = {{Non-Hermiticity of an anomalous superradiant phase}},
  author = {You-Qi Lu and Jun-Ling Wang and Qing-Hu Chen and Yu-Yu Zhang},
  howpublished = {arXiv},
  year = {2026},
  month = oct,
  doi = {10.48550/arxiv.2606.26770},
  eprint = {2606.26770},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2606.26770},
}
RIS
TY  - UNPB
TI  - Non-Hermiticity of an anomalous superradiant phase
AU  - You-Qi Lu
AU  - Jun-Ling Wang
AU  - Qing-Hu Chen
AU  - Yu-Yu Zhang
PY  - 2026
DA  - 2026/10/30
PB  - arXiv
DO  - 10.48550/arxiv.2606.26770
UR  - https://arxiv.org/abs/2606.26770
AB  - We present a Hermitian squeezing-Dicke model as a minimal closed-system setting for non-Hermitian many-body physics. Squeezing generates an effective parity-time (𝒫𝒯) symmetry and exchanges gainy and lossy eigenmodes without dissipation. We identify an anomalous dynamical superradiant phase (DSRP) that exhibits by a mean-field superradiant order in the 𝒫𝒯 symmetry-breaking regime, accompanied by a β„€_2-symmetry-breaking ground-state quantum phase transition. Additionally, it undergoes a 𝒫𝒯-breaking dynamical phase transition at an exceptional point (EP). The excitation energy vanishes near both boundaries, giving critical slowing down. The vacuum photon number is divergent at the ground-state transition but is finite and nonanalytic at the EP, distinguishing the DSRP from the conventional superradiant phase and from a standard dynamical instability. Squeezing causes the coupling phase to act as an artificial magnetic flux, which yields flux-controlled nonreciprocal quantum amplification in the DSRP. Our results offer an alternative pathway to non-Hermitian many-body physics and nonreciprocal quantum amplification in closed Hermitian systems.
ER  -