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Entanglement entropy of 2D conformal quantum critical points: hearing the shape of a quantum drum

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arxiv cond-mat/0605683 v1 pith:CPZSPANM submitted 2006-05-29 cond-mat.str-el cond-mat.mes-hallhep-thquant-ph

classification cond-mat.str-elcond-mat.mes-hallhep-thquant-ph
keywords criticalentanglemententropyquantumpointscentralchargeconformal
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abstract

The entanglement entropy of a pure quantum state of a bipartite system $A \cup B$ is defined as the von Neumann entropy of the reduced density matrix obtained by tracing over one of the two parts. Critical ground states of local Hamiltonians in one dimension have entanglement that diverges logarithmically in the subsystem size, with a universal coefficient that for conformally invariant critical points is related to the central charge of the conformal field theory. We find the entanglement entropy for a standard class of $z=2$ quantum critical points in two spatial dimensions with scale invariant ground state wave functions: in addition to a nonuniversal ``area law'' contribution proportional to the size of the $AB$ boundary, there is generically a universal logarithmically divergent correction. This logarithmic term is completely determined by the geometry of the partition into subsystems and the central charge of the field theory that describes the equal-time correlations of the critical wavefunction.

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Cited by 3 Pith papers

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    Proves exact separability for disconnected subsystems in dimer RK states and exponentially suppressed entanglement for RVB states on arbitrary lattices, with negativity expressed via partition functions.

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