dc.contributor.author | Andersen, Jens Oluf | |
dc.contributor.author | Tranberg, Anders | |
dc.date.accessioned | 2019-10-14T06:39:53Z | |
dc.date.available | 2019-10-14T06:39:53Z | |
dc.date.created | 2012-08-01T12:21:09Z | |
dc.date.issued | 2012 | |
dc.identifier.citation | Journal of High Energy Physics (JHEP). 2012, 2 (8) | nb_NO |
dc.identifier.issn | 1126-6708 | |
dc.identifier.uri | http://hdl.handle.net/11250/2621798 | |
dc.description.abstract | We compute the phase diagram of the quark-meson model at finite temperature, finite baryon chemical potential μ B = 3 μ and constant external magnetic field B, using the functional renormalization group. Our results show that the critical temperature increases as a function of B at μ = 0, but for values μ larger than about 210 − 225 MeV, the opposite behavior is realized. As the magnetic field increases, the critical point (T * , μ *) moves from large μ, small T towards small μ, larger T in the μ-T phase diagram. | nb_NO |
dc.language.iso | eng | nb_NO |
dc.publisher | Springer Nature | nb_NO |
dc.rights | Navngivelse 4.0 Internasjonal | * |
dc.rights.uri | http://creativecommons.org/licenses/by/4.0/deed.no | * |
dc.title | The chiral transition in a magnetic background: Finite density effects and the functional renormalization group | nb_NO |
dc.type | Journal article | nb_NO |
dc.type | Peer reviewed | nb_NO |
dc.description.version | publishedVersion | nb_NO |
dc.source.volume | 2 | nb_NO |
dc.source.journal | Journal of High Energy Physics (JHEP) | nb_NO |
dc.source.issue | 8 | nb_NO |
dc.identifier.doi | 10.1007/JHEP08(2012)002 | |
dc.identifier.cristin | 936890 | |
dc.description.localcode | © SISSA, Trieste, Italy 2012. Open Access CC-BY | nb_NO |
cristin.unitcode | 194,66,20,0 | |
cristin.unitname | Institutt for fysikk | |
cristin.ispublished | true | |
cristin.fulltext | original | |
cristin.qualitycode | 2 | |