Deconfinement transition for nonzero baryon density in the Field Correlator Method
| dc.creator | Simonov, Yu. A. | |
| dc.creator | Trusov, M. A. | |
| dc.date | 2007-03-21 | |
| dc.date | 2007-03-27 | |
| dc.date.accessioned | 2026-07-07T11:02:54Z | |
| dc.date.available | 2026-07-07T11:02:54Z | |
| dc.description | Deconfinement phase transition due to disappearance of confining colorelectric field correlators is described using nonperturbative equation of state. The resulting transition temperature $T_c(μ)$ at any chemical potential $μ$ is expressed in terms of the change of gluonic condensate $ΔG_2$ and absolute value of Polyakov loop $L_{fund} (T_c)$, known from lattice and analytic data, and is in good agreement with lattice data for $ΔG_2 \approx 0.0035 $ GeV$^4$. E.g. $T_c(0) =0.27; 0.19; 0.17$ GeV for $n_f=0,2,3$ respectively. | |
| dc.description | 8 pages, 1 figure, LaTeX2e; some typos corrected | |
| dc.identifier | https://arxiv.org/abs/hep-ph/0703228 | |
| dc.identifier | http://arxiv.org/abs/hep-ph/0703228 | |
| dc.identifier | JETPLett.85:598-601,2007 | |
| dc.identifier | doi:10.1134/S0021364007120028 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/188410 | |
| dc.subject | High Energy Physics - Phenomenology | |
| dc.subject | High Energy Physics - Lattice | |
| dc.subject | Nuclear Experiment | |
| dc.subject | Nuclear Theory | |
| dc.title | Deconfinement transition for nonzero baryon density in the Field Correlator Method | |
| dc.type | text |