Quantum Heisenberg Antiferromagnets versus Nonlinear $σ$ Model Without the Large S Limit
| dc.creator | Zhang, Wei-Min | |
| dc.date | 2001-07-18 | |
| dc.date.accessioned | 2026-07-07T02:42:13Z | |
| dc.date.available | 2026-07-07T02:42:13Z | |
| dc.description | In this letter, I develop a new topologically invariant coherent state path integral for spin systems, and apply it to the quantum Heisenberg model on a square lattice. As a result, the quantum nonlinear $σ$ model for arbitrary values of spin can be directly obtained. The effective coupling constant and spin wave velocity are modified by $g_s= {2\over S}\sqrt{d+{T_Λ\over 2SJ}}$ and $c_s=2JSa \sqrt{d+{T_Λ\over 2SJ}}$, where $T_Λ$ is a natural temperature scale for the reliability of the theory. The formulation can also be extended to other generalized coherent state path integrals. | |
| dc.description | RevTex, 4page, no figure | |
| dc.identifier | https://arxiv.org/abs/cond-mat/0107389 | |
| dc.identifier | http://arxiv.org/abs/cond-mat/0107389 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/18048 | |
| dc.subject | Strongly Correlated Electrons | |
| dc.title | Quantum Heisenberg Antiferromagnets versus Nonlinear $σ$ Model Without the Large S Limit | |
| dc.type | text |