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Annals of Physics

Phase transitions in quantum field theory. I. Phases of the Thirring model

H. S. Sharatchandra, P. Mitra

Published Nov 1, 1979• 2 citations
Publisher
DOI
10.1016/0003-4916(79)90263-x

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Quantum field theory can be a new medium for communication through quantum energy teleportation. We perform a demonstration of quantum energy teleportation with a relativistic fermionic field theory of self-coupled fermions, called the massive Thirring model. Our results reveal that there is a close relationship between the amount of energy teleported and the phase diagram of the theory. In particular, we show that the teleported energy peaks near the phase transition points. Since these results are obtained by measuring the two local subsystems, the noise from the quantum computation can be considerably reduced, allowing for efficient quantum simulations. Moreover, it is a new entanglement-based method that reveals global structure through local measurements.
The standard solution of the Luttinger model (1963) is compared with recent formulations of the Thirring model used in describing Thirring strings. These models may in turn be described by compactified boson models of particular radii. An interesting discrepancy is noted between the apparent radius of the bosons in the Luttinger model and those in the Thirring model. This difference manifests itself in different conformal weights for the fermion fields. The authors resolve this discrepancy by performing an additional rescaling of the Luttinger model bosons. They then examine the enhanced symmetry points that occur in the boson theory at particular values of the radii. In particular, for the Thirring model with two families of spinors, which corresponds to a conformal theory with central extension c=2, one finds an enhanced SU(3) L *SU(3) R symmetry for certain values of the boson radii. This theory is equivalent to the Luttinger model with spin. By examining the response functions for the Luttinger model it is found that the point of SU(3) L *SU(3) R symmetry lies on the Luttinger model phase transition lines.