Reply to “Comment on ‘Z2-slave-spin theory for strongly correlated fermions’”

Andreas Rüegg, Sebastian D. Huber, and Manfred Sigrist
Phys. Rev. B 87, 037102 – Published 2 January 2013

Abstract

We show that the physical subspace in the Z2-slave-spin theory is conserved under the time evolution of the system. Thus, when restricted to the physical subspace, this representation gives a complete and consistent description of the original problem. In addition, we review two known examples from the existing literature in which the projection onto the physical subspace can be relaxed: (i) the noninteracting limit in any dimension at half-filling and (ii) the interacting model in the infinite-dimensional limit at half-filling. In both cases, physical observables are correctly obtained without explicit treatment of the constraints which define the physical subspace. In these examples, correct results are obtained, despite the fact that unphysical states enter the solution.

  • Received 9 July 2012

DOI:https://doi.org/10.1103/PhysRevB.87.037102

©2013 American Physical Society

Authors & Affiliations

Andreas Rüegg

  • Department of Physics, University of California, Berkeley, Berkeley, California 94700, USA

Sebastian D. Huber

  • Department of Condensed Matter Physics, The Weizmann Institute of Science, Rehovot 76100, Israel

Manfred Sigrist

  • Theoretische Physik, ETH Zürich, Zürich CH-8093, Switzerland

Comments & Replies

Comment on “Z2-slave-spin theory for strongly correlated fermions”

Alvaro Ferraz and Evgeny Kochetov
Phys. Rev. B 87, 037101 (2013)

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Original Article

Z2-slave-spin theory for strongly correlated fermions

A. Rüegg, S. D. Huber, and M. Sigrist
Phys. Rev. B 81, 155118 (2010)

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Issue

Vol. 87, Iss. 3 — 15 January 2013

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