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Related papers: An Effective Theory for Baryons in the CFL Phase

200 papers

We study the effect of a non-zero strange quark mass on the color-flavor-locked (CFL) phase of high density quark matter. We have previously shown that for a strange quark mass $m_s\sim m_u^{1/3}\Delta^{2/3}$ the CFL state becomes unstable…

High Energy Physics - Phenomenology · Physics 2008-11-26 Thomas Schaefer

We study the phase diagram of dense quark matter with an emphasis on the role of the strange quark mass. Our approach is based on two effective field theories (EFTs). The first is an EFT that describes quark quasi-particles near the Fermi…

Nuclear Theory · Physics 2016-11-09 Thomas Schaefer

We study the stability of the color-flavor locked (CFL) phase of dense quark matter with regard to the formation of a non-zero Goldstone boson current. We show that an instability appears in the vicinity of the point $\mu_s=\Delta$ which…

High Energy Physics - Phenomenology · Physics 2009-11-11 A. Gerhold , T. Schäfer

We study the structure of mass terms in the effective theory for quasi-particles in QCD at high baryon density. To next-to-leading order in the $1/p_F$ expansion we find two types of mass terms, chirality conserving two-fermion operators…

High Energy Physics - Phenomenology · Physics 2009-11-07 Thomas Schaefer

We study the behavior of Goldstone bosons in color-flavor-locked (CFL) quark matter at nonzero temperature. Chiral symmetry breaking in this phase of cold and dense matter gives rise to pseudo-Goldstone bosons, the lightest of these being…

Nuclear Theory · Physics 2008-11-26 Mark G. Alford , Matt Braby , Andreas Schmitt

We explain how an effective theory of the CFL phase can be used to study the effect of the strange quark mass on the ground state and the excitation spectrum. We also apply the effective theory to the problem of neutrino emission from a CFL…

Nuclear Theory · Physics 2009-11-07 Thomas Schaefer

We study the stability of the kaon condensed color-flavor locked (CFL) phase of dense quark matter with regard to the formation of a non-zero Goldstone boson current. In the kaon condensed phase there is an electrically charged fermion…

High Energy Physics - Phenomenology · Physics 2008-11-26 Andreas Gerhold , Thomas Schaefer , Andrei Kryjevski

At very high densities, QCD is in the color-flavor-locked phase, which is a color-superconducting phase. The diquark condensates break chiral symmetry in the same way as it is broken in vacuum QCD and gives rise to an octet of…

High Energy Physics - Phenomenology · Physics 2015-05-20 Lars E. Leganger

We compute free energy of quark matter at asymptotically high baryon number density in the presence of non zero strange quark mass including dynamics of pseudo Nambu-Goldstone bosons due to chiral symmetry breaking, extending previously…

High Energy Physics - Phenomenology · Physics 2008-11-26 Andrei Kryjevski , Daisuke Yamada

We evaluate several quantities appearing in the effective lagrangian for the color-flavor locked phase of high density QCD using a formalism which exploits the approximate decoupling of fermions with energy negative with respect to the…

High Energy Physics - Phenomenology · Physics 2009-10-31 R. Casalbuoni , R. Gatto , G. Nardulli

We present an effective field theory for high density, low temperature QCD in the crystalline colour superconductive phase (LOFF phase). This interesting phase of QCD is characterized by a gap parameter with a crystalline pattern, breaking…

High Energy Physics - Phenomenology · Physics 2010-11-19 R. Casalbuoni , R. Gatto , M. Mannarelli , G. Nardulli

We calculate the phase diagram of color and electrically neutral quark matter in weak equilibrium using the NJL model at high baryon densities. We extend previous analyses by taking into account the possibility of formation of pseudoscalar…

High Energy Physics - Phenomenology · Physics 2007-05-23 Harmen J. Warringa

We investigate the influence of charged kaon condensation in hadronic sector on the formation of the electron-free charge neutral quark matter of equipartition of three light flavors, i.e., a phenomenon called ``enforced electrical…

High Energy Physics - Phenomenology · Physics 2007-05-23 Youngman Kim , Dong-Pil Min , Mannque Rho

We consider the most general fractional background fluxes in the color, flavor, and baryon number directions, compatible with the faithful action of the global symmetry of a given theory. We call the obstruction to gauging symmetries…

High Energy Physics - Theory · Physics 2020-01-08 Mohamed M. Anber , Erich Poppitz

In neutral cold quark matter that is sufficiently dense that the strange quark mass M_s is unimportant, all nine quarks (three colors; three flavors) pair in a color-flavor locked (CFL) pattern, and all fermionic quasiparticles have a gap.…

High Energy Physics - Phenomenology · Physics 2009-11-10 Mark Alford , Chris Kouvaris , Krishna Rajagopal

We study fermionic quasi-particles in QCD at very high baryon density. In the normal quark matter phase unscreened magnetic gluon exchanges lead to non-Fermi liquid behavior. Non-Fermi liquid effects manifest themselves in low energy Green…

High Energy Physics - Phenomenology · Physics 2009-11-11 Thomas Schaefer

In neutral cold quark matter that is sufficiently dense that the strange quark mass M_s is unimportant, all nine quarks (three colors; three flavors) pair in a color-flavor locked (CFL) pattern, and all fermionic quasiparticles have a gap.…

High Energy Physics - Phenomenology · Physics 2008-11-26 Mark Alford , Chris Kouvaris , Krishna Rajagopal

We offer a diagrammatic derivation of the effective masses of the axial flavor excitations in the electrical and color neutral CFL phase of QCD. In particular we concentrate on the excitations with the quantum numbers of the kaons: we show…

High Energy Physics - Phenomenology · Physics 2009-11-13 Marco Ruggieri

Color-flavor locked (CFL) quark matter at high densities is a color superconductor, which spontaneously breaks baryon number and chiral symmetry. Its low-energy thermodynamic and transport properties are therefore dominated by the H…

Nuclear Theory · Physics 2008-11-26 Mark G. Alford , Matt Braby , Andreas Schmitt

At very high densities, QCD is in the color-flavor locked phase, which is a color-superconducting phase. The diquark condensates break chiral symmetry in the same way as it is broken in vacuum QCD and gives rise to an octet of…

High Energy Physics - Phenomenology · Physics 2010-04-28 Jens O. Andersen , Lars E. Leganger
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