English
Related papers

Related papers: The Color-Superconducting {'}t Hooft Interaction

200 papers

We suggest a scenario where the three light quark flavors are sequentially deconfined under increasing pressure in cold asymmetric nuclear matter, e.g., as in neutron stars. The basis for our analysis is a chiral quark matter model of…

Nuclear Theory · Physics 2008-11-26 David Blaschke , Fredrik Sandin , Thomas Klahn

We study a spin-1 single flavor color superconducting phase which results from a color-spin locking (CSL) interaction in two-flavor quark matter. This phase is particularly interesting for compact star cooling applications since the CSL…

High Energy Physics - Phenomenology · Physics 2009-11-11 D. N. Aguilera , D. Blaschke , M. Buballa , V. L. Yudichev

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. We find two different sources of the infrared cutoff in…

High Energy Physics - Phenomenology · Physics 2017-08-23 E. Gubankova

The phase diagram of strongly interacting matter at non-zero temperature and baryon chemical potential is calculated within a 3-flavor NJL-type quark model with realistic quark masses. The model exhibits spontaneous chiral symmetry breaking…

High Energy Physics - Phenomenology · Physics 2009-11-07 M. Buballa , M. Oertel

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

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 discuss how the co-existence of hyperons, antikaon condensate and color superconducting quark matter in neutron star interior influences the gross properties of compact stars such as, the equation of state and mass-radius relationship.…

Astrophysics · Physics 2009-11-10 Sarmistha Banik , Debades Bandyopadhyay

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 provide a summary of our current knowledge of the phase structure of very dense quark matter. We concentrate on the question how the ground state at asymptotically high density -- color-flavor-locked (CFL) matter -- is modified as the…

Solar and Stellar Astrophysics · Physics 2010-01-19 Thomas Schaefer

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

We investigate the effects of an external magnetic field in the gap structure of a color superconductor with three massless quark flavors. Using an effective theory with four-fermion interactions, inspired by one-gluon exchange, we show…

High Energy Physics - Phenomenology · Physics 2009-11-11 Efrain J. Ferrer , Vivian de la Incera , Cristina Manuel

Color superconductivity of QCD at finite density, temperature and flavor asymmetry is studied within an approximation which the interaction is modeled upon four--fermion interactions. We calculate the thermodynamic potential in the…

High Energy Physics - Phenomenology · Physics 2009-11-07 O. Kiriyama , S. Yasui , H. Toki

The best natural candidates for the realization of color superconductivity are quark stars -not yet confirmed by observation- and the extremely dense cores of compact stars, many of which have very large magnetic fields. To reliably predict…

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

Compact astrophysical objects are a window for the study of strongly interacting nuclear matter given the conditions in their interiors, which are not reproduced in a laboratory environment. Much has been debated about their composition…

High Energy Physics - Phenomenology · Physics 2015-09-23 E. J. Ferrer , V. de la Incera , L. Paulucci

The equation of state for quark matter is derived for a nonlocal, chiral quark model within the mean field approximation. We investigate the effects of a variation of the form factors of the interaction on the phase diagram of quark matter…

High Energy Physics - Phenomenology · Physics 2009-11-10 D. Blaschke , H. Grigorian , D. N. Aguilera , S. Yasui , H. Toki

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

Cold dense quark matter is in a crystalline color superconducting phase wherever pairing occurs between species of quarks with chemical potentials whose difference \delta\mu lies within an appropriate window. If the interaction between…

High Energy Physics - Phenomenology · Physics 2016-09-06 Adam K. Leibovich , Krishna Rajagopal , Eugene Shuster

We investigate the influence of repulsive vector interactions and color superconductivity on the structure of neutron stars using an extended version of the field correlator method (FCM) for the description of quark matter. The hybrid…

In any context in which color superconductivity arises in nature, it is likely to involve pairing between species of quarks with differing chemical potentials. For suitable values of the differences between chemical potentials, Cooper pairs…

High Energy Physics - Phenomenology · Physics 2010-11-19 Mark Alford , Jeffrey Bowers , Krishna Rajagopal

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