Phase diagram of dense two-color QCD within lattice simulations

We present the results of a low-temperature scan of the phase diagram of dense two-color QCD with Nf = 2 quarks. The study is conducted using lattice simulation with rooted staggered quarks. At small chemical potential we observe the hadronic phase, where the theory is in a confining state, chiral s...

Full description

Bibliographic Details
Main Authors: Braguta V.V., Ilgenfritz E.-M., Kotov A.Yu., Molochkov A.V., Nikolaev A.A.
Format: Article
Language:English
Published: EDP Sciences 2017-01-01
Series:EPJ Web of Conferences
Online Access:https://doi.org/10.1051/epjconf/201713707011
id doaj-6be15867891f45ee94815e8a69d654f9
record_format Article
spelling doaj-6be15867891f45ee94815e8a69d654f92021-08-02T10:20:53ZengEDP SciencesEPJ Web of Conferences2100-014X2017-01-011370701110.1051/epjconf/201713707011epjconf_conf2017_07011Phase diagram of dense two-color QCD within lattice simulationsBraguta V.V.Ilgenfritz E.-M.0Kotov A.Yu.Molochkov A.V.1Nikolaev A.A.Joint Institute for Nuclear Research, BLTPSchool of Biomedicine, Far Eastern Federal UniversityWe present the results of a low-temperature scan of the phase diagram of dense two-color QCD with Nf = 2 quarks. The study is conducted using lattice simulation with rooted staggered quarks. At small chemical potential we observe the hadronic phase, where the theory is in a confining state, chiral symmetry is broken, the baryon density is zero and there is no diquark condensate. At the critical point μ = mπ/2 we observe the expected second order transition to Bose-Einstein condensation of scalar diquarks. In this phase the system is still in confinement in conjunction with nonzero baryon density, but the chiral symmetry is restored in the chiral limit. We have also found that in the first two phases the system is well described by chiral perturbation theory. For larger values of the chemical potential the system turns into another phase, where the relevant degrees of freedom are fermions residing inside the Fermi sphere, and the diquark condensation takes place on the Fermi surface. In this phase the system is still in confinement, chiral symmetry is restored and the system is very similar to the quarkyonic state predicted by SU(Nc) theory at large Nc.https://doi.org/10.1051/epjconf/201713707011
collection DOAJ
language English
format Article
sources DOAJ
author Braguta V.V.
Ilgenfritz E.-M.
Kotov A.Yu.
Molochkov A.V.
Nikolaev A.A.
spellingShingle Braguta V.V.
Ilgenfritz E.-M.
Kotov A.Yu.
Molochkov A.V.
Nikolaev A.A.
Phase diagram of dense two-color QCD within lattice simulations
EPJ Web of Conferences
author_facet Braguta V.V.
Ilgenfritz E.-M.
Kotov A.Yu.
Molochkov A.V.
Nikolaev A.A.
author_sort Braguta V.V.
title Phase diagram of dense two-color QCD within lattice simulations
title_short Phase diagram of dense two-color QCD within lattice simulations
title_full Phase diagram of dense two-color QCD within lattice simulations
title_fullStr Phase diagram of dense two-color QCD within lattice simulations
title_full_unstemmed Phase diagram of dense two-color QCD within lattice simulations
title_sort phase diagram of dense two-color qcd within lattice simulations
publisher EDP Sciences
series EPJ Web of Conferences
issn 2100-014X
publishDate 2017-01-01
description We present the results of a low-temperature scan of the phase diagram of dense two-color QCD with Nf = 2 quarks. The study is conducted using lattice simulation with rooted staggered quarks. At small chemical potential we observe the hadronic phase, where the theory is in a confining state, chiral symmetry is broken, the baryon density is zero and there is no diquark condensate. At the critical point μ = mπ/2 we observe the expected second order transition to Bose-Einstein condensation of scalar diquarks. In this phase the system is still in confinement in conjunction with nonzero baryon density, but the chiral symmetry is restored in the chiral limit. We have also found that in the first two phases the system is well described by chiral perturbation theory. For larger values of the chemical potential the system turns into another phase, where the relevant degrees of freedom are fermions residing inside the Fermi sphere, and the diquark condensation takes place on the Fermi surface. In this phase the system is still in confinement, chiral symmetry is restored and the system is very similar to the quarkyonic state predicted by SU(Nc) theory at large Nc.
url https://doi.org/10.1051/epjconf/201713707011
work_keys_str_mv AT bragutavv phasediagramofdensetwocolorqcdwithinlatticesimulations
AT ilgenfritzem phasediagramofdensetwocolorqcdwithinlatticesimulations
AT kotovayu phasediagramofdensetwocolorqcdwithinlatticesimulations
AT molochkovav phasediagramofdensetwocolorqcdwithinlatticesimulations
AT nikolaevaa phasediagramofdensetwocolorqcdwithinlatticesimulations
_version_ 1721234005126283264