Details
| Original language | English |
|---|---|
| Article number | 033302 |
| Journal | Journal of mathematical physics |
| Volume | 58 |
| Issue number | 3 |
| Publication status | Published - 1 Mar 2017 |
| Externally published | Yes |
Abstract
A cornerstone of the theory of phase transitions is the observation that many-body systems exhibiting a spontaneous symmetry breaking in the thermodynamic limit generally show extensive fluctuations of an order parameter in large but finite systems. In this work, we introduce the dynamical analog of such a theory. Specifically, we consider local dissipative dynamics preparing an equilibrium steady-state of quantum spins on a lattice exhibiting a discrete or continuous symmetry but with extensive fluctuations in a local order parameter. We show that for all such processes, there exist asymptotically stationary symmetry-breaking states, i.e., states that become stationary in the thermodynamic limit and give a finite value to the order parameter. We give results both for discrete and continuous symmetries and explicitly show how to construct the symmetry-breaking states. Our results show in a simple way that, in large systems, local dissipative dynamics satisfying detailed balance cannot uniquely and efficiently prepare states with extensive fluctuations with respect to local operators. We discuss the implications of our results for quantum simulators and dissipative state preparation.
ASJC Scopus subject areas
- Physics and Astronomy(all)
- Statistical and Nonlinear Physics
- Mathematics(all)
- Mathematical Physics
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In: Journal of mathematical physics, Vol. 58, No. 3, 033302, 01.03.2017.
Research output: Contribution to journal › Article › Research › peer review
}
TY - JOUR
T1 - Emergence of spontaneous symmetry breaking in dissipative lattice systems
AU - Wilming, Henrik
AU - Kastoryano, Michael J.
AU - Werner, Albert H.
AU - Eisert, Jens
N1 - Funding Information: This work has been supported by the ERC (TAQ), the EU (RAQUEL, AQuS, SIQS), the COST network, the DFG (Grant Nos. CRC 183 and EI 519/7-1), and the Studienstiftung des Deutschen Volkes. M.J.K. was supported by the Carlsberg foundation and the Villum foundation.
PY - 2017/3/1
Y1 - 2017/3/1
N2 - A cornerstone of the theory of phase transitions is the observation that many-body systems exhibiting a spontaneous symmetry breaking in the thermodynamic limit generally show extensive fluctuations of an order parameter in large but finite systems. In this work, we introduce the dynamical analog of such a theory. Specifically, we consider local dissipative dynamics preparing an equilibrium steady-state of quantum spins on a lattice exhibiting a discrete or continuous symmetry but with extensive fluctuations in a local order parameter. We show that for all such processes, there exist asymptotically stationary symmetry-breaking states, i.e., states that become stationary in the thermodynamic limit and give a finite value to the order parameter. We give results both for discrete and continuous symmetries and explicitly show how to construct the symmetry-breaking states. Our results show in a simple way that, in large systems, local dissipative dynamics satisfying detailed balance cannot uniquely and efficiently prepare states with extensive fluctuations with respect to local operators. We discuss the implications of our results for quantum simulators and dissipative state preparation.
AB - A cornerstone of the theory of phase transitions is the observation that many-body systems exhibiting a spontaneous symmetry breaking in the thermodynamic limit generally show extensive fluctuations of an order parameter in large but finite systems. In this work, we introduce the dynamical analog of such a theory. Specifically, we consider local dissipative dynamics preparing an equilibrium steady-state of quantum spins on a lattice exhibiting a discrete or continuous symmetry but with extensive fluctuations in a local order parameter. We show that for all such processes, there exist asymptotically stationary symmetry-breaking states, i.e., states that become stationary in the thermodynamic limit and give a finite value to the order parameter. We give results both for discrete and continuous symmetries and explicitly show how to construct the symmetry-breaking states. Our results show in a simple way that, in large systems, local dissipative dynamics satisfying detailed balance cannot uniquely and efficiently prepare states with extensive fluctuations with respect to local operators. We discuss the implications of our results for quantum simulators and dissipative state preparation.
UR - http://www.scopus.com/inward/record.url?scp=85016164404&partnerID=8YFLogxK
U2 - 10.1063/1.4978328
DO - 10.1063/1.4978328
M3 - Article
AN - SCOPUS:85016164404
VL - 58
JO - Journal of mathematical physics
JF - Journal of mathematical physics
SN - 0022-2488
IS - 3
M1 - 033302
ER -