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Universality classes split by strong and weak symmetries

Jongjun M. Lee, Myung-Joong Hwang, Igor Boettcher

Abstract

Dissipative phase transitions are strongly shaped by the symmetries of the Liouvillian, yet the quantitative impact of weak and strong symmetries on critical behavior has remained unclear. We study a squeezed-photon model with single- and two-photon losses, realizing weak and strong symmetries in the simplest possible setting. The two symmetries exhibit identical Gaussian static fluctuations, whereas the order parameter and the asymptotic decay rate display distinct scaling behaviors. Our one-loop Keldysh analysis, together with cumulant-expansion numerics, reveals sharply different critical scaling with respect to the thermodynamic scaling parameter. This establishes that weak and strong symmetries lead to distinct dynamical universality classes despite originating from the same symmetry group in the closed system. Our results provide a clear quantitative demonstration that strong symmetries fundamentally reshape dissipative criticality.

Universality classes split by strong and weak symmetries

Abstract

Dissipative phase transitions are strongly shaped by the symmetries of the Liouvillian, yet the quantitative impact of weak and strong symmetries on critical behavior has remained unclear. We study a squeezed-photon model with single- and two-photon losses, realizing weak and strong symmetries in the simplest possible setting. The two symmetries exhibit identical Gaussian static fluctuations, whereas the order parameter and the asymptotic decay rate display distinct scaling behaviors. Our one-loop Keldysh analysis, together with cumulant-expansion numerics, reveals sharply different critical scaling with respect to the thermodynamic scaling parameter. This establishes that weak and strong symmetries lead to distinct dynamical universality classes despite originating from the same symmetry group in the closed system. Our results provide a clear quantitative demonstration that strong symmetries fundamentally reshape dissipative criticality.
Paper Structure (32 equations, 2 figures, 2 tables)

This paper contains 32 equations, 2 figures, 2 tables.

Figures (2)

  • Figure 1: Schematic illustrations of (a) the system, (b) the phase diagram as a function of the two-photon driving strength $\lambda$, and (c) the loop diagrams relevant to the quartic-order corrections to the retarded Green function. The single-photon loss ($\kappa_{1}$) is present only for the weak parity symmetry. N and SR denote the normal and superradiant phases, respectively.
  • Figure 2: Numerical results from the cumulant expansion. (a) Number fluctuation $\delta n$, (b) $\mathrm{Re}[\delta m]$, and (c) $\mathrm{Im}[\delta m]$ at the critical driving strength $\lambda_c$ as functions of the two-photon loss rate $\kappa_2$ for weak (W) and strong (S) parity symmetries. Black lines indicate power-law fits. (d) Rescaled number fluctuation $\kappa_2^{1/2(2/3)} \delta n$ versus $\kappa_2^{-1/2(-2/3)} |\lambda-\lambda_c|$ in the superradiant phase for weak (strong) parity symmetries. Colors denote different values of $\kappa_2$. The collapse of data points onto a single curve confirms Eq. (\ref{['Eq_Uni_Scal_1']}).