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Related papers: On Mass Spectrum in SQCD. Unequal quark masses

200 papers

We analyze (using a chiral effective Lagrangian model) the scalar and pseudoscalar meson mass spectrum of QCD at finite temperature, above the chiral transition at $T_c$, looking, in particular, for signatures of a possible breaking of the…

High Energy Physics - Phenomenology · Physics 2014-10-15 Enrico Meggiolaro

We study the effect of a non-zero strange quark mass on the color-flavor-locked (CFL) phase of high density quark matter. We have previously shown that for a strange quark mass $m_s\sim m_u^{1/3}\Delta^{2/3}$ the CFL state becomes unstable…

High Energy Physics - Phenomenology · Physics 2008-11-26 Thomas Schaefer

The ground state of dense up and down quark matter under local and global charge neutrality conditions with $\beta$-equilibrium has at least four possibilities: normal, regular 2SC, gapless 2SC phases, and mixed phase composed of 2SC phase…

High Energy Physics - Phenomenology · Physics 2007-05-23 Mei Huang , Igor Shovkovy

We compute the static-light baryon spectrum with N_f = 2 flavors of sea quarks using Wilson twisted mass lattice QCD. As light valence quarks we consider quarks, which have the same mass as the sea quarks with corresponding pion masses in…

High Energy Physics - Lattice · Physics 2019-08-13 Marc Wagner , Christian Wiese

The dynamics in QCD with different number of fermion flavors N_f is discussed. The emphasis is on the description of the conformal phase transition with respect to N_f separating a phase with no confinement and chiral symmetry breaking and…

High Energy Physics - Phenomenology · Physics 2007-05-23 V. A. Miransky

Considering four-point correlation functions of color-singlet quark bilinears, we investigate, in the large-$N_{\mathrm{c}}$ limit of QCD, the subleading diagrams that involve, in the $s$-channel of meson-meson scattering amplitudes,…

High Energy Physics - Phenomenology · Physics 2017-12-20 Wolfgang Lucha , Dmitri Melikhov , Hagop Sazdjian

I explore the rich phase diagram of two-flavor QCD as a function of the quark masses. The theory involves three parameters, including one that is CP violating. As the masses vary, regions of both first and second order transitions are…

High Energy Physics - Phenomenology · Physics 2011-02-03 Michael Creutz

Instantons generate strong non-perturbative interactions between quarks. In the vacuum, these interactions lead to chiral symmetry breaking and generate constituent quark masses on the order of 300-400 MeV. The observation that the same…

High Energy Physics - Phenomenology · Physics 2009-10-31 R. Rapp , T. Schaefer , E. V. Shuryak , M. Velkovsky

We describe the interplay of two nonperturbative phenomena which should take place in the chirally invariant deconfined phase of QCD matter at finite density and T=0: (i) Cooper-pair quark-quark ground-state condensation in appropriate…

High Energy Physics - Phenomenology · Physics 2007-05-23 Jiri Hosek

The spectrum of meson and diquark excitations of dense color neutral cold quark matter is investigated in the framework of a 2-flavored Nambu--Jona-Lasinio type model, including a quark $\mu$- and color $\mu_8$ chemical potential. It was…

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

The talk is an introduction into diquark condensation phenomena which occur in QCD at high energy density. They are driven by instantons and instanton-antiinstanton pairs (or ``molecules''), which generate attraction in some qq channels. A…

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

The phase diagram of three-flavor quark matter under compact star constraints is investigated within a Nambu--Jona-Lasinio model. Local color and electric charge neutrality is imposed for beta-equilibrated superconducting quark matter. The…

High Energy Physics - Phenomenology · Physics 2009-09-29 D. Blaschke , S. Fredriksson , H. Grigorian , A. M. "Oztas , F. Sandin

The present lecture is devoted to embedding the approximate genuine harmonic oscillator structure of valence q qbar mesons and in more detail the q q q configurations for up,down,strange - flavored baryons in Q C D for three light flavors…

High Energy Physics - Theory · Physics 2015-06-19 Peter Minkowski

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

A good agreement between a flux tube-based quark model of light baryons (strange and nonstrange) and the $1/N_c$ expansion mass formula has been found in previous studies. In the present work a larger connection is established between the…

High Energy Physics - Phenomenology · Physics 2008-11-26 C. Semay , F. Buisseret , F. Stancu

We show that the quark condensates for the two light up and down flavors can have significantly different values in the hadronic phase at nonzero temperature, baryon and isospin chemical potentials. We quantify this difference using a…

High Energy Physics - Phenomenology · Physics 2007-05-23 D. Toublan

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 present a lattice QCD determination of light quark masses with three sea-quark flavours ($N_f = 2+1$). Bare quark masses are known from PCAC relations in the framework of CLS lattice computations with a non-perturbatively improved…

High Energy Physics - Lattice · Physics 2020-02-26 Mattia Bruno , Isabel Campos , Patrick Fritzsch , Jonna Koponen , Carlos Pena , David Preti , Alberto Ramos , Anastassios Vladikas

Quarks and antiquarks carry color and electric charges and belong to the color-triplet $3$ group and the color-antitriplet $\bar 3$ group respectively. The product groups of $3$ and $\bar 3$ consist of the color-singlet $1$ and the…

High Energy Physics - Phenomenology · Physics 2026-01-09 Cheuk-Yin Wong

Recently, there have been reports that the chirally restored phase of QCD is effectively symmetric under $U(N_f) \times U(N_f)$ rather than $SU(N_f)\times SU(N_f)$. We supplement their argument by including the contributions from…

High Energy Physics - Phenomenology · Physics 2009-12-30 Su H. Lee , T. Hatsuda