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Related papers: Meson current in the CFL phase

200 papers

We explore the phase diagram of neutral quark matter at high baryon density as a function of the temperature T and the strange quark mass Ms. At T=0, there is a sharp distinction between the insulating color-flavor locked (CFL) phase, which…

High Energy Physics - Phenomenology · Physics 2014-11-18 Kenji Fukushima , Chris Kouvaris , Krishna Rajagopal

We investigate the consequences of enforcing local color neutrality on the color superconducting phases of quark matter by utilizing the Nambu-Jona-Lasinio model supplemented by diquark and the t'Hooft six-fermion interactions. In neutrino…

High Energy Physics - Phenomenology · Physics 2009-11-07 Andrew W. Steiner , Sanjay Reddy , Madappa Prakash

We recently argued that as the density of quark matter decreases, there is a continuous transition from the color-flavor-locked (CFL) phase to a gapless "gCFL" phase. The reason is the growing importance of the strange quark mass, and the…

High Energy Physics - Phenomenology · Physics 2017-08-23 Mark Alford , Chris Kouvaris , Krishna Rajagopal

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

Considering the density dependence of quark masses, we investigate the color-flavor-locked matter and its stability relative to the ( unpaired ) strange quark matter. We find that, when the current mass of strange quark $m_s$ is small, the…

High Energy Physics - Phenomenology · Physics 2014-11-18 Xiao-Bing Zhang , Xue-Qian Li

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 construct the U_L(3) x U_R(3) effective lagrangian which encodes the dynamics of the low energy pseudoscalar excitations in the Color-Flavor-Locking superconducting phase of QCD at finite quark density. We include the effects of…

High Energy Physics - Phenomenology · Physics 2009-10-31 Cristina Manuel , Michel H. G. Tytgat

Thermal emission rates and mean free paths of photons in a color-flavor locked (CFL) phase of quark matter at high densities and moderate temperatures are evaluated. Our calculations are based on a low-energy effective theory for CFL matter…

High Energy Physics - Phenomenology · Physics 2009-11-10 C. Vogt , R. Rapp , R. Ouyed

I discuss some aspects of recent developments in color superconductivity in high density quark matter. I calculate the Cooper pair gap and the critical points at high density, where magnetic gluons are not screened. The ground state of high…

High Energy Physics - Phenomenology · Physics 2007-05-23 Deog Ki Hong

We study weak interactions involving Goldstone bosons in the neutral kaon condensed phase of color flavor locked quark matter. We calculate the rates for the dominant processes that contribute to the neutrino mean free p ath and to neutrino…

Nuclear Theory · Physics 2009-11-10 Sanjay Reddy , Mariusz Sadzikowski , Motoi Tachibana

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 argue that in the color-flavor-locking (CFL) superconducting phase classical soliton solutions can exist, whose excitations should be interpreted as states formed by a quark (or an antiquark) and condensed diquarks. This finding extends…

High Energy Physics - Phenomenology · Physics 2009-11-10 R. Casalbuoni , G. Nardulli

This paper is devoted to the study of some aspects of the instability of two flavor color superconductive quark matter. We find that, beside color condensates, the Goldstone boson related to the breaking of $U(1)_A$ suffers of a velocity…

High Energy Physics - Phenomenology · Physics 2008-11-26 R. Gatto , M. Ruggieri

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 calculate the bulk viscosity of color-superconducting quark matter in the color-flavor-locked (CFL) phase. We assume that the lightest bosons are the superfluid mode H and the kaons K0 and K+, and that there is no kaon condensate. We…

Nuclear Theory · Physics 2008-11-26 Mark G. Alford , Matt Braby , Sanjay Reddy , Thomas Schaefer

We investigate the effects of the dynamical formation of the chiral condensates on color superconducting phases under the electric and color neutrality constraints at vanishing temperature. We shall show that the phase appearing next to the…

High Energy Physics - Phenomenology · Physics 2009-11-10 H. Abuki , M. Kitazawa , T. Kunihiro

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

At asymptotic high density and low temperature quarks form Cooper pairs in a color-flavor locked (CFL) configuration. The diquark condensates break spontaneously the baryon symmetry, and this fact makes the CFL phase also superfluid. At low…

High Energy Physics - Phenomenology · Physics 2009-06-25 Cristina Manuel

The spectrum of meson and diquark excitations of dense quark matter is considered in the framework of the Nambu -- Jona-Lasinio model with three types of massless quarks in the presense of a quark number chemical potential $\mu$. We…

High Energy Physics - Phenomenology · Physics 2008-11-26 D. Ebert , K. G. Klimenko , V. L. Yudichev

The equilibrium between the so-called 2SC and CFL phases of strange quark matter at high densities is investigated in the framework of a simple schematic model of the NJL type. Equal densities are assumed for quarks $u,d$ and $s$. The 2SC…

Nuclear Theory · Physics 2015-05-30 Henrik Bohr , Prafulla K. Panda , Constança Providência , João da Providência