Thermal Operator Representation of Finite Temperature Graphs II
| dc.creator | Brandt, Fernando T. | |
| dc.creator | Das, Ashok | |
| dc.creator | Espinosa, Olivier | |
| dc.creator | Frenkel, Josif | |
| dc.creator | Perez, Silvana | |
| dc.date | 2006-01-30 | |
| dc.date | 2006-02-09 | |
| dc.date.accessioned | 2026-07-07T11:27:22Z | |
| dc.date.available | 2026-07-07T11:27:22Z | |
| dc.description | Using the mixed space representation, we extend our earlier analysis to the case of Dirac and gauge fields and show that in the absence of a chemical potential, the finite temperature Feynman diagrams can be related to the corresponding zero temperature graphs through a thermal operator. At non-zero chemical potential we show explicitly in the case of the fermion self-energy that such a factorization is violated because of the presence of a singular contact term. Such a temperature dependent term which arises only at finite density and has a quadratic mass singularity cannot be related, through a regular thermal operator, to the fermion self-energy at zero temperature which is infrared finite. Furthermore, we show that the thermal radiative corrections at finite density have a screening effect for the chemical potential leading to a finite renormalization of the potential. | |
| dc.description | 13 pages, 4 figures. Revised version (minor changes) accepted for publication in Phys. Rev. D | |
| dc.identifier | https://arxiv.org/abs/hep-th/0601224 | |
| dc.identifier | http://arxiv.org/abs/hep-th/0601224 | |
| dc.identifier | Phys.Rev.D73:065010,2006 | |
| dc.identifier | doi:10.1103/PhysRevD.73.065010 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/196129 | |
| dc.subject | High Energy Physics - Theory | |
| dc.subject | High Energy Physics - Phenomenology | |
| dc.title | Thermal Operator Representation of Finite Temperature Graphs II | |
| dc.type | text |