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Related papers: Evaluating the Gapless Color-Flavor Locked Phase

200 papers

Using flow equations, we derive an effective quark-quark interaction and obtain the coupled set of gap equations for the condensates of the CFL phase of massless $N_f=3$ dense QCD. The formalism developed here enables one to consider more…

High Energy Physics - Phenomenology · Physics 2009-11-07 E. Gubankova

Thermal color superconducting phase transitions in three-flavor quark matter at high baryon density are investigated in the Ginzburg-Landau (GL) approach. We constructed the GL potential near the boundary with a normal phase by taking into…

High Energy Physics - Phenomenology · Physics 2009-11-10 K. Iida , T. Matsuura , M. Tachibana , T. Hatsuda

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

We investigate the effects of realistic quark masses and local color neutrality on quark pairing in the three-flavor Polyakov--Nambu--Jona-Lasinio model. While prior studies have indicated the presence of light flavor quark (2SC) or…

High Energy Physics - Phenomenology · Physics 2013-07-16 Philip D. Powell , Gordon Baym

Owing to the emergence of attractive interactions between quarks, color superconductivity is expected to occur, with the color-flavor-locked (CFL) phase favored at high densities. This work investigates the absolute stability of…

High Energy Physics - Phenomenology · Physics 2026-05-20 Wen-Li Yuan , Bikai Gao

Strange quark matter in a color flavor locked (CFL) state can be the true ground state of hadronic matter for a much wider range of the parameters of the model (the gap of the QCD Cooper pairs $\Delta$, the strange quark mass $m_s$ and the…

Astrophysics · Physics 2008-11-26 G. Lugones , J. E. Horvath

The structure of the phase diagram of strongly interacting matter at moderate densities is calculated within a 3-flavor NJL-type quark model with realistic quark masses. We focus on the influence of the selfconsistently determined effective…

High Energy Physics - Phenomenology · Physics 2007-05-23 M. Oertel , M. Buballa

We analyze the spectrum of the massive states for the color flavor locked phase (CFL) of QCD. We show that the vector mesons have a mass of the order of the color superconductive gap $\Delta$. We also see that the excitations associated…

High Energy Physics - Phenomenology · Physics 2015-06-25 A. D. Jackson , F. Sannino

We calculate the spectral densities of electric and magnetic gluons at zero temperature in color-superconducting quark matter in the color-flavor-locking (CFL) phase. We find a collective excitation, a plasmon, at energies smaller than two…

High Energy Physics - Phenomenology · Physics 2007-05-23 H. Malekzadeh , Dirk H. Rischke

Color-flavor locked (CFL) quark matter expels color-magnetic fields due to the Meissner effect. One of these fields carries an admixture of the ordinary abelian magnetic field and therefore flux tubes may form if CFL matter is exposed to a…

High Energy Physics - Phenomenology · Physics 2020-08-07 Alexander Haber , Andreas Schmitt

QCD superconductors in the color-flavor-locked (CFL) phase support excitations (generalized mesons) that can be described as pairs of particles or holes (rather than particle-hole) around a gapped Fermi surface. In weak coupling and to…

High Energy Physics - Phenomenology · Physics 2008-11-26 Mannque Rho , Edward Shuryak , Andreas Wirzba , Ismail Zahed

The stability of color-flavor locked (CFL) strangelets is studied in the three-flavor Nambu--Jona-Lasinio model. We consider all quark flavors to be massless, for simplicity. By making use of the multiple reflection expansion, we explicitly…

High Energy Physics - Phenomenology · Physics 2010-11-05 O. Kiriyama

We consider the phase diagram of QCD at very high baryon density and at zero temperature in the presence of a strong magnetic field. The state of matter at such high densities and low temperatures is believed to be a phase known as the…

High Energy Physics - Phenomenology · Physics 2015-07-08 Srimoyee Sen

At nuclear matter density, electrically neutral strongly interacting matter in weak equilibrium is made of neutrons, protons and electrons. At sufficiently high density, such matter is made of up, down and strange quarks in the color-flavor…

High Energy Physics - Phenomenology · Physics 2009-11-07 Mark Alford , Krishna Rajagopal , Sanjay Reddy , Frank Wilczek

We present a detailed study of the recently proposed gapless color superconductivity in neutral two-flavor quark matter in beta-equilibrium at zero as well as at finite temperature. We clarify the nature of the fermionic quasiparticles, and…

High Energy Physics - Phenomenology · Physics 2010-04-05 Mei Huang , Igor Shovkovy

We consider the effect of a six-fermion interaction of the {'}t Hooft form in the quark-quark channel on the ground state of matter at finite density. The coupling constant for this new term is varied within the limits suggested by…

High Energy Physics - Phenomenology · Physics 2011-07-19 Andrew W. Steiner

I investigate some of the inert phases in three-flavor, spin-zero color-superconducting quark matter: the CFL phase (the analogue of the B phase in superfluid $^3\rm He$), the A and A* phases, and the 2SC and sSC phases. I compute the…

High Energy Physics - Phenomenology · Physics 2009-11-11 H. Malekzadeh

The simplest pattern of color superconductivity involves BCS pairing between up and down quarks. We argue that this ``2SC'' phase will not arise within a compact star. A macroscopic volume of quark matter must be electrically neutral and…

High Energy Physics - Phenomenology · Physics 2009-11-07 Mark Alford , Krishna Rajagopal

We calculate the Debye and Meissner masses and investigate chromomagnetic instability associated with the gapless color superconducting phase changing the strange quark mass $M_s$ and the temperature $T$. Based on the analytical study, we…

High Energy Physics - Phenomenology · Physics 2009-11-11 Kenji Fukushima

We investigate the phases of dense QCD matter at finite temperature with Dyson-Schwinger equations for the quark propagator for N_f=2+1 flavors. For the gluon propagator we take a fit to quenched lattice data and add quark-loop effects…

High Energy Physics - Phenomenology · Physics 2013-07-30 Daniel Müller , Michael Buballa , Jochen Wambach