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Related papers: Generalized Pions in Dense QCD

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We investigate color superconducting phases of cold quark matter at densities relevant for the interiors of compact stars. At these densities, electrically neutral and weak-equilibrated quark matter can have unequal numbers of up, down, and…

High Energy Physics - Phenomenology · Physics 2013-05-29 Jeffrey A. Bowers

At sufficiently high densities, cold dense three-flavor quark matter is in the color-flavor locked (CFL) phase, in which all nine quarks pair in a particularly symmetric fashion. Once the heaviness of the strange quark (mass $m_s$) and the…

High Energy Physics - Phenomenology · Physics 2008-11-26 Krishna Rajagopal , Andreas Schmitt

As recently shown, the ground state of dense QCD matter in a strong magnetic field is an inhomogeneous condensate of neutral pions which was named Chiral Soliton Lattice (CSL) phase in analogy with a state present for chiral magnets. We…

High Energy Physics - Phenomenology · Physics 2019-05-14 Helena Kolešová

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

We study pseudoscalar meson excitations in the color-flavor locked phase within a Nambu-Jona-Lasinio-type model by calculating diquark loops.

High Energy Physics - Phenomenology · Physics 2008-11-26 Verena Werth , Michael Buballa , Micaela Oertel

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 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

The formfactors of B_1 -> pi and D_1 -> pi transitions, where B_1(D_1) is the 1^+ P-wave -> Q gamma_{\nu}\gamma_5q meson state, are calculated in the framework of the light cone QCD. Furthermore these formfactors are compared with the pole…

High Energy Physics - Phenomenology · Physics 2009-10-28 T. M. Aliev , A. Ozpineci , M. Savci

We present an initiatory study of quark helicity flip generalized parton distributions (GPDs) in n_f=2 lattice QCD, based on clover-improved Wilson fermions for a large number of coupling constants and pion masses. Quark helicity flip GPDs…

High Energy Physics - Lattice · Physics 2008-11-26 M. Gockeler , Ph. Hagler , R. Horsley , D. Pleiter , P. E. L. Rakow , A. Schafer , G. Schierholz , J. M. Zanotti

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

We study the low energy effective action for the collective modes of the color flavor locked phase of QCD. This phase of matter has long been known to be a superfluid because by picking a phase its order parameter breaks the quark-number…

High Energy Physics - Phenomenology · Physics 2015-03-17 Roberto Anglani , Massimo Mannarelli , Marco Ruggieri

The properties of cold and dense quark matter have been the subject of extensive investigation, especially in the last decade. Unfortunately, we still lack of a complete understanding of the properties of matter in these conditions. One…

High Energy Physics - Phenomenology · Physics 2009-06-25 Massimo Mannarelli

Quantum chromodynamics (QCD) at finite temperature, $T$, and quark chemical potential, $\mu$, has a rich phase structure: at low $T$ and low $\mu$, the Nambu-Goldstone (NG) phase with nearly massless pions is realized by the dynamical…

High Energy Physics - Phenomenology · Physics 2015-05-14 Tetsuo Hatsuda , Kenji Maeda

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

Lattice QCD is used to calculate the potential between a static quark and anti-quark in the presence of a finite density of pi^+'s. Correlation functions of multiple pi^+'s are used in conjunction with Wilson-loop correlators to determine…

High Energy Physics - Lattice · Physics 2009-02-23 William Detmold , Martin J. Savage

The last few years have seen significant experimental progress in characterizing the copper-based hole-doped high temperature superconductors in the regime of low hole density, p. Quantum oscillations, NMR, X-ray, and STM experiments have…

Strongly Correlated Electrons · Physics 2016-08-01 Debanjan Chowdhury , Subir Sachdev

We discuss a universal non-equilibrium enhancement of long-wavelength Goldstone bosons induced by quenches to the broken phase in Model G -- the dynamical universality class of an $O(4)$-antiferromagnet and the chiral phase transition in…

High Energy Physics - Phenomenology · Physics 2025-12-15 Adrien Florio , Eduardo Grossi , Aleksas Mazeliauskas , Alexander Soloviev , Derek Teaney

We investigate the positivity of the Euclidean path integral measure for low-energy modes in dense fermionic matter. We show that the sign problem usually associated with fermions is absent if one considers only low-energy degrees of…

High Energy Physics - Phenomenology · Physics 2017-08-23 D. K. Hong , S. D. H. Hsu

The self-energies and the spectral densities of longitudinal and transverse gluons at zero temperature in the color-flavor-locked (CFL) phase are calculated. There appears a collective excitation, a light plasmon, at energies smaller than…

High Energy Physics - Phenomenology · Physics 2008-11-26 H. Malekzadeh , Dirk H. Rischke

We study color superconductivity in external magnetic field. We discuss the reason why the mixing angles in color-flavor locked (CFL) and two-flavor superconductivity (2SC) phases are different despite the fact that the CFL gap goes to the…

High Energy Physics - Phenomenology · Physics 2009-10-31 E. V. Gorbar
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