{ "id": "1703.06411", "version": "v1", "published": "2017-03-19T10:02:36.000Z", "updated": "2017-03-19T10:02:36.000Z", "title": "Phases of circle-compactified QCD with adjoint fermions at finite density", "authors": [ "Takuya Kanazawa", "Mithat Ünsal", "Naoki Yamamoto" ], "comment": "16 pages, 11 figures", "categories": [ "hep-th", "hep-lat", "hep-ph" ], "abstract": "We study chemical-potential dependence of confinement and mass gap in QCD with adjoint fermions in spacetime with one spatial compact direction. By calculating the one-loop effective potential for the Wilson line in the presence of chemical potential, we show that a center-symmetric phase and a center-broken phase alternate when the chemical potential in unit of the compactification scale is increased. In the center-symmetric phase we use semiclassical methods to show that photons in the magnetic bion plasma acquire a mass gap that grows with the chemical potential as a result of anisotropic interactions between monopole-instantons. For the neutral fermionic sector which remains gapless perturbatively, there are two possibilities at non-perturbative level. Either to remain gapless (unbroken global symmetry), or to undergo a novel superfluid transition through a four-fermion interaction (broken global symmetry). If the latter is the case, this leads to an energy gap of quarks proportional to a new nonperturbative scale $L^{-1}\\exp[-1/(g^4 \\mu L)]$, where $L$ denotes the circumference of $S^1$, the low-energy is described as a Nambu-Goldstone mode associated with the baryon number, and there exists a new type of BEC-BCS crossover of the diquark pairing as a function of the compactification scale at small chemical potential.", "revisions": [ { "version": "v1", "updated": "2017-03-19T10:02:36.000Z" } ], "analyses": { "keywords": [ "adjoint fermions", "finite density", "circle-compactified qcd", "chemical potential", "mass gap" ], "note": { "typesetting": "TeX", "pages": 16, "language": "en", "license": "arXiv", "status": "editable" } } }