Density resummation of perturbation series in a pion gas to leading order in chiral perturbation theory
| dc.creator | Krivoruchenko, M. I. | |
| dc.creator | Fuchs, C. | |
| dc.creator | Martemyanov, B. V. | |
| dc.creator | Faessler, Amand | |
| dc.date | 2005-05-10 | |
| dc.date | 2006-10-26 | |
| dc.date.accessioned | 2026-07-07T11:04:45Z | |
| dc.date.available | 2026-07-07T11:04:45Z | |
| dc.description | The mean field (MF) approximation for the pion matter, being equivalent to the leading ChPT order, involves no dynamical loops and, if self-consistent, produces finite renormalizations only. The weight factor of the Haar measure of the pion fields, entering the path integral, generates an effective Lagrangian $δ\mathcal{L}_{H}$ which is generally singular in the continuum limit. There exists one parameterization of the pion fields only, for which the weight factor is equal to unity and $δ\mathcal{L}_{H}=0$, respectively. This unique parameterization ensures selfconsistency of the MF approximation. We use it to calculate thermal Green functions of the pion gas in the MF approximation as a power series over the temperature. The Borel transforms of thermal averages of a function $\mathcal{J}(χ^αχ^α)$ of the pion fields $χ^α$ with respect to the scalar pion density are found to be $\frac{2}{\sqrtπ}\mathcal{J}(4t)$. The perturbation series over the scalar pion density for basic characteristics of the pion matter such as the pion propagator, the pion optical potential, the scalar quark condensate $<{\bar{q}}q>$, the in-medium pion decay constant ${\tilde{F}}$, and the equation of state of pion matter appear to be asymptotic ones. These series are summed up using the contour-improved Borel resummation method. The quark scalar condensate decreases smoothly until $T_{max}\simeq 310$ MeV. The temperature $T_{max}$ is the maximum temperature admissible for thermalized non-linear sigma model at zero pion chemical potentials. The estimate of $T_{max}$ is above the chemical freeze-out temperature $T\simeq 170$ MeV at RHIC and above the phase transition to two-flavor quark matter $T_{c} \simeq 175$ MeV, predicted by lattice gauge theories. | |
| dc.description | Replaced with revised and extended version. Results are compared to lattice gauge theories. 16 pages REVTeX, 13 eps figures | |
| dc.identifier | https://arxiv.org/abs/hep-ph/0505083 | |
| dc.identifier | http://arxiv.org/abs/hep-ph/0505083 | |
| dc.identifier | Phys.Rev.D74:125019,2006 | |
| dc.identifier | doi:10.1103/PhysRevD.74.125019 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/188998 | |
| dc.subject | High Energy Physics - Phenomenology | |
| dc.subject | High Energy Physics - Lattice | |
| dc.subject | Nuclear Theory | |
| dc.title | Density resummation of perturbation series in a pion gas to leading order in chiral perturbation theory | |
| dc.type | text |