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Related papers: Neutral Color Superconductivity and Pseudo-Goldsto…

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The properties of pseudoscalar bosonic excitations in the color-flavor locked phase at moderate densities are studied within a model of the Nambu--Jona-Lasinio type. Our previous analysis is extended to Goldstone bosons with hidden flavor…

High Energy Physics - Phenomenology · Physics 2009-02-26 Verena Kleinhaus , Michael Buballa

Spin-one color superconductor is a viable candidate phase of dense matter in the interiors of compact stars. Its low-energy excitations will influence the transport properties of such matter and thus have impact on late-stage evolution of…

High Energy Physics - Phenomenology · Physics 2014-11-20 Tomas Brauner , Jin-yi Pang , Qun Wang

We study the Bethe-Salpeter equations for spin zero diquark composites in the color superconducting phase of N_f=2 cold dense QCD. The explicit form of the spectrum of the diquarks, containing an infinite tower of narrow (at high density)…

High Energy Physics - Phenomenology · Physics 2009-10-31 V. A. Miransky , I. A. Shovkovy , L. C. R. Wijewardhana

We study the low energy phase structure of SU(2) gauge theories in three-dimensional spacetime, at finite baryon density. The pseudoreality of representations of SU(2) permits an analytic study of a real baryon chemical potential, and the…

High Energy Physics - Phenomenology · Physics 2009-11-07 Gerald V. Dunne , Shinsuke M. Nishigaki

We have simulated two-colour four-flavour QCD at non-zero chemical potential $\mu$ for quark number. Simulations were performed on $8^4$ and $12^3 \times 24$ lattices. Clear evidence was seen for the formation of a colourless diquark…

High Energy Physics - Lattice · Physics 2014-11-17 J. B. Kogut , D. K. Sinclair , S. J. Hands , S. E. Morrison

We examine the spectrum of 2-colour lattice QCD with 4 continuum flavours at a finite chemical potential ($\mu$) for quark-number, on a $12^3 \times 24$ lattice. First we present evidence that the system undergoes a transition to a state…

High Energy Physics - Lattice · Physics 2009-11-10 J. B. Kogut , D. Toublan , D. K. Sinclair

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 show that the third Goldstone mode, which emerges in binary condensates at phase-separation, persists to higher inter-species interaction for density profiles where one component is surrounded on both sides by the other component. This…

Quantum Gases · Physics 2014-01-23 Arko Roy , S. Gautam , D. Angom

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

I clarify how the concept of quark-hadron continuity, which was previously considered in the context of the asymptotic color-flavor locked phase with ideal three-flavor symmetry, is applied to two-flavor matter. Our observation is that…

High Energy Physics - Phenomenology · Physics 2021-02-03 Yuki Fujimoto

QCD predicts matter at high density should exhibit color superconductivity. We review briefly several pertinent properties of color superconductivity and then discuss how baryons are realized in color superconductors. Especially, we explain…

High Energy Physics - Phenomenology · Physics 2009-03-16 Deog Ki Hong

QCD superconductors in the color-flavor-locked (CFL) phase sustain light Goldstone modes (that will be referred to as generalized pions) that can be described as pairs of particle and/or hole excitations around a gapped Fermi surface. In…

High Energy Physics - Phenomenology · Physics 2007-05-23 Mannque Rho , Andreas Wirzba , Ismail Zahed

We consider an extended Nambu--Jona-Lasinio model including both (q \bar q)- and (qq)-interactions with two light-quark flavors in the presence of a single (quark density) chemical potential. In the color superconducting phase of the quark…

High Energy Physics - Phenomenology · Physics 2009-11-10 D. Blaschke , D. Ebert , K. G. Klimenko , M. K. Volkov , V. L. Yudichev

It is quite plausible that color superconductivity occurs in the inner regions of neutron stars. At the same time, it is known that strong magnetic fields exist in the interior of these compact objects. In this paper we discuss some…

Astrophysics · Physics 2008-11-26 Efrain J. Ferrer , Vivian de la Incera

A phase diagram for a 2D metal with variable carrier density has been derived. It consists of a normal phase, where the order parameter is absent; a so-called ``abnormal normal'' phase where this parameter is also absent but the mean number…

Superconductivity · Physics 2009-10-30 Valery P. Gusynin , Vadim M. Loktev , Sergei G. Sharapov

The spectrum of meson and diquark excitations in cold color-superconducting (2SC) quark matter is investigated under local color and electric neutrality constraints with $\beta$-equilibrium. A 2-flavored Nambu--Jona-Lasinio type model…

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

Owing to extremely large band gap of 5.5 eV and high thermal conductivity, diamond is recognized as the most important semiconductor. The superconductivity of polycrystalline diamond has always been reported, but there are also many…

Superconductivity · Physics 2024-03-04 Shisheng Lin , Xutao Yu , Minhui Yang , Huikai Zhong , Jiarui Guo

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

Color superconductivity in QCD breaks the SU(3) color gauge group down to SU(2), inducing masses in five of the eight gluons. This is a dynamical Higgs effect, in which the diquark condensate acts as the vacuum expectation value of a…

High Energy Physics - Phenomenology · Physics 2009-10-31 G. W. Carter , D. Diakonov

Many models of meta-stable supersymmetry (SUSY) breaking lead to a very light scalar pseudo-Nambu Goldstone boson (PNGB), P, associated with spontaneous breakdown of a baryon number like symmetry in the hidden sector. Current particle…

High Energy Physics - Phenomenology · Physics 2010-01-08 Tom Banks , Howard E. Haber