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Springer proceedings in physics

Symmetry Breaking in a Quantum Double-Well Chain

James E. Gubernatis, David K Campbell, Xidi Wang

Published Jan 1, 1992• 0 citations
Publisher
DOI
10.1007/978-3-642-84821-6_26

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The quantum ground-state and excitation properties of two independent chains of pseudospins (two-level systems) interacting with the same bosonic field are theoretically investigated. Each chain is coupled to a different quadrature of the field, leading to two independent symmetry breakings for increasing values of the two collective spin-boson interaction constants ${\ensuremath{\Omega}}_{C}$ and ${\ensuremath{\Omega}}_{I}$. A phase diagram is provided in the plane (${\ensuremath{\Omega}}_{C}$,${\ensuremath{\Omega}}_{I}$), with four phases that can be characterized by the complex bosonic coherence of the ground states and can be manipulated via geometric Berry effects. In particular, when ${\ensuremath{\Omega}}_{C}$ and ${\ensuremath{\Omega}}_{I}$ are both larger than two critical values, the fundamental subspace has a fourfold degeneracy. Finite-size properties are shown for both critical and ultrastrong values of ${\ensuremath{\Omega}}_{C}$ and ${\ensuremath{\Omega}}_{I}$. Possible implementations in superconducting quantum circuits are detailed.
In this paper, we apply the method of breaking quantum double symmetries to some cases of defect-mediated melting. The formalism allows for a systematic classification of possible defect condensates and the subsequent confinement and/or liberation of other degrees of freedom. We also show that the breaking of a double symmetry may well involve a (partial) restoration of an original symmetry. A detailed analysis of a number of simple but representative examples is given, where we focus on systems with global internal and external (space) symmetries. We start by rephrasing some of the well-known cases involving an Abelian defect condensate, such as the Kosterlitz-Thouless transition and one-dimensional melting, in our language. Then we proceed to the non-Abelian case of a hexagonal crystal, where the hexatic phase is realized if translational defects condense in a particular rotationally invariant state. Other conceivable phases are also described in our framework.