Bosonization of non-relativistic fermions on a circle: Tomonaga's problem revisited
| dc.creator | Dhar, Avinash | |
| dc.creator | Mandal, Gautam | |
| dc.date | 2006-03-20 | |
| dc.date.accessioned | 2026-07-07T10:46:14Z | |
| dc.date.available | 2026-07-07T10:46:14Z | |
| dc.description | We use the recently developed tools for an exact bosonization of a finite number $N$ of non-relativistic fermions to discuss the classic Tomonaga problem. In the case of noninteracting fermions, the bosonized hamiltonian naturally splits into an O$(N)$ piece and an O$(1)$ piece. We show that in the large-N and low-energy limit, the O$(N)$ piece in the hamiltonian describes a massless relativistic boson, while the O$(1)$ piece gives rise to cubic self-interactions of the boson. At finite $N$ and high energies, the low-energy effective description breaks down and the exact bosonized hamiltonian must be used. We also comment on the connection between the Tomonaga problem and pure Yang-Mills theory on a cylinder. In the dual context of baby universes and multiple black holes in string theory, we point out that the O$(N)$ piece in our bosonized hamiltonian provides a simple understanding of the origin of two different kinds of nonperturbative O$(e^{-N})$ corrections to the black hole partition function. | |
| dc.description | latex, 28 pages, 5 epsf figures | |
| dc.identifier | https://arxiv.org/abs/hep-th/0603154 | |
| dc.identifier | http://arxiv.org/abs/hep-th/0603154 | |
| dc.identifier | Phys.Rev.D74:105006,2006 | |
| dc.identifier | doi:10.1103/PhysRevD.74.105006 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/183166 | |
| dc.subject | High Energy Physics - Theory | |
| dc.subject | Statistical Mechanics | |
| dc.title | Bosonization of non-relativistic fermions on a circle: Tomonaga's problem revisited | |
| dc.type | text |