English
Related papers

Related papers: Stable Pentaquarks from Strange Chiral Multiplets

200 papers

The strange-anticharmed Pentaquark is a $uud\bar{c}s$ or $udd\bar{c}s$ five-quark baryon that is expected to be either a narrow resonance, or possibly even stable against strong and electromagnetic decay. We describe this hyperon here, its…

High Energy Physics - Phenomenology · Physics 2008-11-26 M. A. Moinester , D. Ashery , L. G. Landsberg , H. J. Lipkin

A general study of pentaquarks built with four quarks in a L=1 state and an antiquark in S-wave shows that several of such states are forbidden by a selection rule, which holds in the limit of flavour symmetry, to decay into a baryon and a…

High Energy Physics - Phenomenology · Physics 2009-11-10 F. Buccella , P. Sorba

We show that, in a model based exclusively on constituent-quark degrees of freedom interacting via a potential, the full axial current is conserved if the spectrum of \bar QQ states contains a massless pseudoscalar. The current conservation…

High Energy Physics - Phenomenology · Physics 2008-11-26 Wolfgang Lucha , Dmitri Melikhov , Silvano Simula

Quark condensate and pseudoscalar decay constant in the chiral limit are the principal order parameters of spontaneous chiral symmetry breaking in QCD. Yet their three flavor values are still only weakly constrained by analyses using…

High Energy Physics - Phenomenology · Physics 2014-04-01 Marián Kolesar , Jiří Novotný

We construct a self-consistent holographic QCD model which can realize two most important phenomena of QCD, i.e. chiral symmetry breaking and confinement. The model is formulated in the framework of graviton-dilaton-scalar system, where the…

High Energy Physics - Phenomenology · Physics 2015-06-11 Danning Li , Mei Huang , Qi-Shu Yan

We introduce a random matrix model with the symmetries of QCD with two colors at nonzero isospin and baryon chemical potentials and temperature. We analyze its phase diagram and find phases with condensation of pion and diquark states in…

High Energy Physics - Phenomenology · Physics 2009-11-10 B. Klein , D. Toublan , J. J. M. Verbaarschot

In a diquark-diquark-antiquark picture of the pentaquark we study the decay $\Theta \rightarrow K^{+} n$ within the framework of QCD sum rules. After evaluation of the relevant three-point function, we extract the coupling $g_{\Theta nK}$…

High Energy Physics - Phenomenology · Physics 2009-11-11 M. Eidemüller , F. S. Navarra , M. Nielsen , R. Rodrigues da Silva

Starting from the approximate symmetries of QCD, namely chiral symmetry for light quarks and spin and flavor symmetry for heavy quarks, we investigate the low-energy properties of heavy hadrons. For this purpose we construct a consistent…

High Energy Physics - Phenomenology · Physics 2007-05-23 D. Ebert , T. Feldmann

The experimental signature of an S=+1 baryon of mass 1540 MeV and width 10-25 MeV has led to speculation that this is an exotic baryon consisting of 4 quarks and 1 antiquark lying at the top of a $\bar{10}$ SU(3) multiplet. The observed…

High Energy Physics - Phenomenology · Physics 2007-05-23 Steven Golbeck , Mikhail Savrov

We address the old difficulty in accommodating the scalar quark-antiquark confining potential together with chiral symmetry breaking. We develop a quark confining potential inspired in the QCD scalar flux tube. The coupling to quarks…

High Energy Physics - Phenomenology · Physics 2007-05-23 P. Bicudo , G. M. Marques

A chiral effective theory of scalar and vector diquarks is formulated, which is based on $SU(3)_R\times SU(3)_L$ chiral symmetry and includes interactions between scalar and vector diquarks with one or two mesons. We find that the diquark…

High Energy Physics - Phenomenology · Physics 2023-04-26 Yonghee Kim , Makoto Oka , Daiki Suenaga , Kei Suzuki

We introduce coupled channels of Bethe-Salpeter mesons both in the boundstate equation for mesons and in the mass gap equation for chiral symmetry. Consistency is insured by the Ward Identities for axial currents, which preserve the…

Nuclear Theory · Physics 2010-11-15 Pedro Bicudo

Using the picture of the flux tube model, we propose that the $\Theta_5$ pentaquark as the first candidate of the three-dimensional non-planar hadron with the extremely stable diamond structure. The up and down quarks lie at the corners of…

High Energy Physics - Phenomenology · Physics 2009-11-10 Xing-Chang Song , Shi-Lin Zhu

We review, clarify, and extend the notion of color-flavor locking. We present evidence that for three degenerate flavors the qualitative features of the color-flavor locked state, reliably predicted for high density, match the expected…

High Energy Physics - Phenomenology · Physics 2009-10-31 Thomas Schaefer , Frank Wilczek

Soft-wall models in AdS/QCD generally have dilaton and scalar fields that vary with the fifth-dimension coordinate. These fields can be parameterized to yield hadron mass spectra with linear radial trajectories and to incorporate…

High Energy Physics - Phenomenology · Physics 2010-06-01 J. I. Kapusta , T. Springer

Above the chiral symmetry restoration crossover around T_{ch} ~ 155 MeV a new regime arises in QCD, a stringy fluid, which is characterized by an approximate chiral spin symmetry of the thermal partition function. This symmetry is not a…

High Energy Physics - Lattice · Physics 2023-05-31 L. Ya. Glozman

The LHCb collaboration has recently announced the discovery of two hidden-charm pentaquark states with also strange quark content, $P_{cs}(4338)$ and $P_{cs}(4459)$; its analysis points towards having both hadrons isospin equal to zero and…

High Energy Physics - Phenomenology · Physics 2023-11-03 Gang Yang , Jialun Ping , Jorge Segovia

We study renormalized quenched strong-coupling QED in four dimensions in arbitrary covariant gauge. Above the critical coupling leading to dynamical chiral symmetry breaking, we show that there is no finite chiral limit. This behaviour is…

High Energy Physics - Phenomenology · Physics 2010-03-04 Frederick T. Hawes , Tom Sizer , Anthony G. Williams

A diquark model previously formulated to describe exotic mesons is extended to dibaryons. In the model, dibaryons containing only light quarks are unbound. The $H$ dibaryon, consisting of $uuddss$ quarks, is unstable by about 90 MeV or…

High Energy Physics - Phenomenology · Physics 2007-05-23 D. B. Lichtenberg , R. Roncaglia , E. Predazzi

A dynamically broken hadron supersymmetry appears to exist as a consequence of QCD. The reasons for the supersymmetry appear most transparently in the framework of the constituent quark model with a diquark approximation to two quarks.…

High Energy Physics - Phenomenology · Physics 2007-05-23 D. B. Lichtenberg