Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Revista Mexicana de Física

Pseudo-spin dynamical symmetry

Jerry Paul Draayer, C. Bahri, S. A. Moszkowski

Published Jan 1, 1992• 0 citations
OpenAlex

Related papers

Pseudo-spin symmetry in the Hubbard model

J. P. Wallington, James F. Annett

We present a hidden SU(2) ‘pseudo-spin’ symmetry of the half-filled Hubbard model, relating superconducting and charge orderings. Using an appropriate functional integral representation, we show the consequences of this symmetry for the quasiparticle excitation spectrum.

Philosophical Magazine B•Nov 1, 1997•3 citations

Reformulation of spin pseudoclassical dynamics

V. Pažma, Peter Prešnajder

Czechoslovak Journal of Physics•Aug 1, 1992•0 citations

Symmetry of the Spin Systems

Roman Boča

Elsevier eBooks•Jan 1, 2012•0 citations

Symmetry classification of spin-orbit-coupled spinor Bose-Einstein condensates

Zhi-Fang Xu, Yuki Kawaguchi, Li You +1 more

We develop a symmetry classification scheme to find ground states of pseudo-spin-$\frac{1}{2}$, spin-1, and spin-2 spin-orbit-coupled spinor Bose-Einstein condensates and show that as the SO(2) symmetry of simultaneous spin and space rotations is broken into discrete cyclic groups, various types of lattice structures emerge in the absence of a lattice potential. Examples include two different kagome lattices for pseudo-spin-$\frac{1}{2}$ condensates and a nematic vortex lattice in which uniaxial and biaxial spin textures align alternatively for spin-2 condensates. For the pseudo-spin-$\frac{1}{2}$ system, although mean-field states always break time-reversal symmetry, there exists a time-reversal invariant many-body ground state, which is fragmented and expected to be observed in a microcondensate.

arXiv:1203.2005•Physical Review A•Sep 26, 2012•74 citations

Symmetry adapted states for Hubbard clusters

O. Tjernberg

The application of spin, pseudo spin and space group symmetry to find symmetry adapted states for the square planar Hubbard model is discussed. An approach based on pseudo spin configurations and the application of Young tableaux to the permutation group is presented. The method is illustrated for the case of a 4*4 cluster and the complete classification of the states for this cluster is given. It is shown that the linear dimension of the largest matrix block is reduced by three orders of magnitude by application of the above symmetries.

Journal of Mathematical Physics•Dec 1, 1998•2 citations

Pseudo-Spin-Coherent States

Monique Combescure, Didier Robert

Theoretical and mathematical physics•Jan 1, 2012•0 citations
We develop a symmetry classification scheme to find ground states of pseudo-spin-12\frac{1}{2}21​, spin-1, and spin-2 spin-orbit-coupled spinor Bose-Einstein condensates and show that as the SO(2) symmetry of simultaneous spin and space rotations is broken into discrete cyclic groups, various types of lattice structures emerge in the absence of a lattice potential. Examples include two different kagome lattices for pseudo-spin-12\frac{1}{2}21​ condensates and a nematic vortex lattice in which uniaxial and biaxial spin textures align alternatively for spin-2 condensates. For the pseudo-spin-12\frac{1}{2}21​ system, although mean-field states always break time-reversal symmetry, there exists a time-reversal invariant many-body ground state, which is fragmented and expected to be observed in a microcondensate.
The application of spin, pseudo spin and space group symmetry to find symmetry adapted states for the square planar Hubbard model is discussed. An approach based on pseudo spin configurations and the application of Young tableaux to the permutation group is presented. The method is illustrated for the case of a 4*4 cluster and the complete classification of the states for this cluster is given. It is shown that the linear dimension of the largest matrix block is reduced by three orders of magnitude by application of the above symmetries.