{ "id": "1511.00031", "version": "v1", "published": "2015-10-30T21:11:35.000Z", "updated": "2015-10-30T21:11:35.000Z", "title": "Large-$N$ pion scattering at finite temperature: the $f_0(500)$ and chiral restoration", "authors": [ "Santiago Cortes", "Angel Gomez Nicola", "John Morales" ], "comment": "24 pages, 12 figures", "categories": [ "hep-ph" ], "abstract": "We consider the $O(N+1)/O(N)$ Non-Linear Sigma Model for large $N$ as an effective theory for low-energy QCD at finite temperature $T$, in the chiral limit. At $T=0$ this formulation provides a good description of scattering data in the scalar channel and generates dynamically the $f_0(500)$ pole, the pole position lying within experimental determinations. Previous $T=0$ results with this model are updated using newer analysis of pion scattering data. We calculate the pion scattering amplitude at finite $T$ and show that it satisfies exactly thermal unitarity, which had been assumed but not formally proven in previous works. We discuss the main differences with the $T=0$ result and we show that one can define a proper renormalization scheme with $T=0$ counterterms such that the renormalized amplitude can be chosen to depend only on a few parameters. Next, we analyze the behaviour of the $f_0(500)$ pole at finite $T$, which is consistent with chiral symmetry restoration when the scalar susceptibility is saturated by the $f_0(500)$ state, in a second-order transition scenario and in accordance with lattice and theoretical analysis.", "revisions": [ { "version": "v1", "updated": "2015-10-30T21:11:35.000Z" } ], "analyses": { "keywords": [ "finite temperature", "chiral restoration", "non-linear sigma model", "second-order transition scenario", "satisfies exactly thermal unitarity" ], "publication": { "doi": "10.1103/PhysRevD.93.036001" }, "note": { "typesetting": "TeX", "pages": 24, "language": "en", "license": "arXiv", "status": "editable", "inspire": 1402372 } } }