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  • Letter

False vacuum decay in quantum spin chains

Gianluca Lagnese1,2, Federica Maria Surace1,3, Márton Kormos4,5, and Pasquale Calabrese1,2,3

  • 1SISSA, via Bonomea 265, 34136 Trieste, Italy
  • 2INFN, Sezione di Trieste, 34136 Trieste, Italy
  • 3International Centre for Theoretical Physics (ICTP), Strada Costiera 11, 34151 Trieste, Italy
  • 4Budapest University of Technology and Economics, Department of Theoretical Physics, 1111 Budapest, Budafoki út 8, Hungary
  • 5MTA-BME Quantum-Dynamics and Correlations Research Group (ELKH), Budapest University of Technology and Economics, 1111 Budapest, Budafoki út 8, Hungary

Phys. Rev. B 104, L201106 – Published 12 November, 2021

DOI: https://doi.org/10.1103/PhysRevB.104.L201106

Abstract

The false vacuum decay has been a central theme in physics for half a century with applications to cosmology and to the theory of fundamental interactions. This fascinating phenomenon is even more intriguing when combined with the confinement of elementary particles. Due to the astronomical timescales involved, the research has so far focused on theoretical aspects of this decay. The purpose of this Letter is to show that the false vacuum decay is accessible to current optical experiments as quantum analog simulators of spin chains with confinement of the elementary excitations, which mimic the high energy phenomenology but in one spatial dimension. We study the nonequilibrium dynamics of the false vacuum in a quantum Ising chain and in an XXZ ladder. The false vacuum is the metastable state that arises in the ferromagnetic phase of the model when the symmetry is explicitly broken by a longitudinal field. This state decays through the formation of “bubbles” of true vacuum. Using infinite volume time evolving block decimation (iTEBD) simulations, we are able to study the real-time evolution in the thermodynamic limit and measure the decay rate of local observables. We find that the numerical results agree with the theoretical prediction that the decay rate is exponentially small in the inverse of the longitudinal field.

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