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Superalgebraic solution to the mean-field Hubbard model

Arianna Montorsi, Mario Rasetti, A. I. Solomon

Published Jan 1, 1989• 1 citation
OpenAlex

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A simple version of the Bardeen-Cooper-Schrieffer (BCS)-type mean-field theory for the $t\ensuremath{-}J$ model is developed. The present approach rigorously treats the constraint of no doubly occupied states and invokes two local order parameters to implement spontaneous breaking of the global $\mathrm{U}(1)\ifmmode\times\else\texttimes\fi{}\mathrm{U}(1)$ symmetry. This is achieved by identifying the Hubbard operators with generators of the $\mathrm{SU}(2|1)$ superalgebra in the fundamental representation and employing the ensuing ${\mathrm{CP}}^{1|1}$ parametrization for dynamical variables. As a result, an improved phase diagram ${T}_{c}(\ensuremath{\delta})$ in the paramagnetic phase is obtained.

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Nikolay M. Plakida, V. Yu. Yushankhaï

We show that the phase diagram and the odd p-wave quasiparticle gap for spinless fermions obtained in the paper by Kochetov and Mierzejewski for the $t\ensuremath{-}J$ model are artifacts of the adopted spin-charge separation treated in mean field approximation, while the critical remarks concerning the theory of exchange superconducting pairing derived within the Hubbard operator approach are misleading.

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Mean‐Field Theory of an Extended Hubbard Model

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physica status solidi (b)•Oct 1, 1989•0 citations
A simple version of the Bardeen-Cooper-Schrieffer (BCS)-type mean-field theory for the $t\ensuremath{-}J$ model is developed. The present approach rigorously treats the constraint of no doubly occupied states and invokes two local order parameters to implement spontaneous breaking of the global $\mathrm{U}(1)\ifmmode\times\else\texttimes\fi{}\mathrm{U}(1)$ symmetry. This is achieved by identifying the Hubbard operators with generators of the SU(2∣1)\mathrm{SU}(2|1)SU(2∣1) superalgebra in the fundamental representation and employing the ensuing CP1∣1{\mathrm{CP}}^{1|1}CP1∣1 parametrization for dynamical variables. As a result, an improved phase diagram ${T}_{c}(\ensuremath{\delta})$ in the paramagnetic phase is obtained.