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Related papers: The hexaquark-flavoured antiK-N-N state computed m…

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We analyse the decay $\Theta_s(1/2^+)\to NK$ in a non-relativistic Fock space description using three and five constituent quarks for the nucleon and the pentaquark, respectively. Following Jaffe and Wilczek \cite{jw}, we assume that…

High Energy Physics - Phenomenology · Physics 2009-11-11 Dmitri Melikhov

The Strange Quark matter (SQM) hypothesis states that at extreme pressure and density conditions a new ground state of matter would arise, in which half of the \textit{down} quarks become strange quarks. If true, it would mean that at least…

High Energy Astrophysical Phenomena · Physics 2023-04-05 A. Bernardo , L. Paulucci , L. M. de Sá , J. E. Horvath

Following a recent suggestion by Weinberg, we use the large-N expansion in QCD to discuss the decay amplitudes of tetraquarks into ordinary mesons as well as their mixing properties. We find that the flavor structure of the tetraquark is a…

High Energy Physics - Phenomenology · Physics 2013-09-04 Marc Knecht , Santiago Peris

We present a very general argument that the analogue of a heavy pentaquark (a state with the quantum numbers of a baryon combined with an additional light quark and a heavy antiquark) must exist as a particle stable under strong…

High Energy Physics - Phenomenology · Physics 2016-09-06 Thomas D. Cohen , Paul M. Hohler , Richard F. Lebed

The splittings between positive parity pentaquarks containing a single heavy (c,b) antiquark and four light (u,d) quarks are investigated in models having spin-dependent interactions generated by either effective Goldstone boson exchange or…

High Energy Physics - Phenomenology · Physics 2009-11-10 K. Maltman

We present the formalism for a new generation of unquenched quark models in which quark-antiquark pair effects are taken into account in an explicit form via a microscopic QCD-inspired quark-antiquark creation mechanism. No truncation in…

High Energy Physics - Phenomenology · Physics 2017-08-23 E. Santopinto , R. Bijker

At RHIC the cross section for c-cbar production will be large enough such that approximately 10 pairs will be produced in each central collision. If a region of deconfined quarks and gluons is subsequently formed, one would expect that the…

High Energy Physics - Phenomenology · Physics 2008-11-26 R L Thews , M Schroedter , J Rafelski

Cooled down and diluted quark-gluon matter is considered. A possibility of condensation of multiquark clusters with zero N-alities is discussed.

High Energy Physics - Lattice · Physics 2015-06-25 Vladimir K. Petrov

We construct the complete set of positive parity pentaquarks, which correspond in the quark model to {\bar s} q^{Nc+1} states with one unit of orbital angular momentum L=1. In the large Nc limit they fall into the K=1/2 and K=3/2 irreps…

High Energy Physics - Phenomenology · Physics 2008-11-26 Dan Pirjol , Carlos Schat

We use Nuclear Magnetic Resonance (NMR) to experimentally generate a bound entangled (more precisely: pseudo bound entangled) state, i.e. a quantum state which is non-distillable but nevertheless entangled. Our quantum system consists of…

Quantum Physics · Physics 2010-11-08 H. Kampermann , X. Peng , D. Bruss , D. Suter

We discuss recent theoretical developments concerning the description of the production and decay of heavy quarks and colored scalars in the framework of nonrelativistic QCD.

High Energy Physics - Phenomenology · Physics 2007-05-23 Pedro Ruiz-Femenia , Andre Hoang

I summarize the current status of the comparison between experiment and the predictions of the NRQCD factorization approach to quarkonium decay and production. I also present the results of some recent calculations and theoretical…

High Energy Physics - Phenomenology · Physics 2017-08-23 Geoffrey T. Bodwin

The color number $N_c$-dependence of the interplay between quark-antiquark condensates $<\bar{q}q>$ and diquark condensates $<qq>$ in vacuum in two-flavor four-fermion interaction models is researched. The results show that the $G_S$-$H_S$…

High Energy Physics - Theory · Physics 2009-08-25 Bang-Rong Zhou

For the case of two light flavors we propose the stringy description of the system consisting of two heavy and three light quarks, with the aim of exploring the quark organization inside the system and its low-lying Born-Oppenheimer…

High Energy Physics - Phenomenology · Physics 2023-02-15 Oleg Andreev

Classical color fields produced by the small-x wave functions of colliding ultrarelativistic nuclei have been numerically computed. We set up the framework for computing the production of small-mass quark-antiquark pairs in these color…

High Energy Physics - Phenomenology · Physics 2007-05-23 F. Gelis , K. Kajantie , T. Lappi

We used an effective Lagrangian approach to investigate the production of the anticharmed pentaquark state $P_{\bar{c}s}^{(*)-}$ with the minimal quark content $\bar{c}sudd$ in the $\Lambda_b^0$ decay and its decay into the $\Lambda…

High Energy Physics - Phenomenology · Physics 2025-01-27 Shi-Dong Liu , Xiao-Yun Wang , Xiao-Hai Liu , Gang Li

For the case of two light flavors we propose the stringy description of the system made of one heavy and one light quark-antiquark pair, with the aim of exploring the two lower-lying Born-Oppenheimer potentials as a function of a separation…

High Energy Physics - Phenomenology · Physics 2023-06-27 Oleg Andreev

The structure of $K^-$-condensed hypernuclei, which may be produced in the laboratory in strangeness-conserving processes, is investigated using an effective chiral Lagrangian for the kaon-baryon interaction, combined with a nonrelativistic…

Nuclear Theory · Physics 2008-11-26 Takumi Muto

Multiquark systems such as tetraquarks, pentaquarks and hexaquarks states are studied as di-hadronic molecules in a nonrelativistic model. The masses of several di-hadronic states using a molecular interaction provided by asymptotic…

High Energy Physics - Phenomenology · Physics 2008-11-26 Ajay Kumar Rai , J N Pandya , P C Vinodkumar

Many known models, which generally use a factorization hypothesis, give a poor account of the decays B into J/psi + K(*). Usually there is a free overall factor, which is fit to the data, so that tests of the models rely upon ratios. The…

High Energy Physics - Phenomenology · Physics 2009-09-25 Carl E. Carlson , J. Milana