English
Related papers

Related papers: Pentaquarks in the Jaffe-Wilczek approximation

200 papers

The light scalar mesons below 1 GeV as tetraquark states are studied in the framework of the flux-tube model, the multi-body confinement instead of the additive two-body confinement is used. From the calculated results, we find that the…

High Energy Physics - Phenomenology · Physics 2015-06-04 C. R. Deng , J. L. Ping , F. Wang

We determine the masses of the light and the strange quarks in the MS-bar-scheme using our high-statistics lattice simulation of QCD with dynamical Wilson fermions. For each of our three sea quarks we have analyzed our data at five…

High Energy Physics - Phenomenology · Physics 2009-10-30 H. Hoeber

The pentaquark state recently discovered has been studied with three quark models which either fit the nucleon spin structure or the $NN$ scattering. A minimum $\Theta^+$ mass of 1620 MeV is obtained both for the ${1/2}^\pm$ state. The…

High Energy Physics - Phenomenology · Physics 2008-11-26 Jialun Ping , Di Qing , Fan Wang , T. Goldman

We present a new lattice QCD analysis of heavy-quark pseudoscalar-pseudoscalar correlators, using gluon configurations from the MILC collaboration that include vacuum polarization from $u$, $d$, $s$ and $c$~quarks($n_f=4$). We extract new…

High Energy Physics - Lattice · Physics 2015-03-25 Bipasha Chakraborty , C. T. H. Davies , G. C. Donald , R. J. Dowdall , B. Galloway , P. Knecht , J. Koponen , G. P. Lepage , C. McNeile

We present a systematic study of the effectiveness of light quark mass reweighting. This method allows a single lattice QCD ensemble, generated with a specific value of the dynamical light quark mass, to be used to determine results for…

High Energy Physics - Lattice · Physics 2013-03-14 Qi Liu , Norman H. Christ , Chulwoo Jung

We studied the $D\bar{D}^\ast/\bar{D}D^\ast$, $D^\ast\bar{D}^\ast$, $\bar{D}_s D^\ast/\bar{D}_s^\ast D$, $B\bar{B}^\ast/\bar{B}B^\ast$ and $B^\ast\bar{B}^\ast$ di-hadron interactions in chiral effective field theory ($\chi$EFT) up to the…

High Energy Physics - Phenomenology · Physics 2023-02-20 Bo Wang , Lu Meng , Shi-Lin Zhu

Hadron masses are subject to few MeV corrections arising from QED interactions, almost entirely arising from the electric charge of the valence quarks. The QED effects include both self-energy contributions and interactions between the…

High Energy Physics - Lattice · Physics 2020-11-25 D. Hatton , C. T. H. Davies , G. P. Lepage

As our recent quark model calculation~\cite{Noh:2023fdy} suggests a strong possibility of a compact $T_{cc}$ that closely reproduces experimental mass, we have a strong incentive to extend our work to investigate the possible compact…

High Energy Physics - Phenomenology · Physics 2023-08-02 Woosung Park , Sungsik Noh

By taking into light the discovery of pentaquark structures like $P_{\psi s}^\Lambda(4338)^0$, $P_c(4380)$ and $P_c(4450)$, we performed the spectroscopy of hidden-bottom pentaquarks. By utilizing special unitary representations, we…

High Energy Physics - Phenomenology · Physics 2024-10-10 Ankush Sharma , Alka Upadhyay

Hadron spectroscopy is a powerful tool for testing the standard model and for the search of new physics. In this work, we create a tetraquark model from a di-meson interaction inspired by Jacobi coordinates. We consider mesons as thick…

High Energy Physics - Phenomenology · Physics 2021-01-12 J. A. Lesteiro-Tejeda , D. A. Ramírez-Zaldívar , C. E. Gracía-Trápaga , F. Guzmán-Martínez

Possibility of an axial vector isoscalar tetraquark $ud\bar{s}\bar{s}$ is discussed. If a $f_1$ meson in the mass region $1.4-1.5$ GeV consists of four quarks $ns\bar{n}\bar{s}$, the mass of the isoscalar…

Nuclear Theory · Physics 2008-11-26 Yoshiko Kanada-En'yo , Osamu Morimatsu , Tetsuo Nishikawa

We derive an upper bound on the mass difference between the $\Xi^*$ and $\Theta^+$ pentaquarks which are the manifestly exotic members of the $SU(3)_f$ antidecuplet. The derivation is based on simple assumptions about $SU(3)_f$ symmetry…

High Energy Physics - Phenomenology · Physics 2009-11-10 Marek Karliner , Harry. J. Lipkin

The interaction of the charmed baryon and the anticharmed meson is assumed to be realized by exchanging a scalar meson of $f_0(500)$, and then these systems are studied by solving the Schrodinger equation, respectively. When the pentaquarks…

High Energy Physics - Phenomenology · Physics 2025-07-01 Bao-Xi Sun

The mass of the top quark is measured using a sample of t t-bar candidate events with one electron or muon and at least four jets in the final state, collected by CMS in pp collisions at sqrt(s) = 7 TeV at the LHC. A total of 5174 candidate…

High Energy Physics - Experiment · Physics 2013-03-19 The CMS Collaboration

In this article, we construct the scalar-diquark-axialvector-diquark-antiquark type interpolating currents, and study the masses and pole residues of the $J^{P}=\frac{3}{2}^{\pm}$ hidden-charmed pentaquark states with the QCD sum rules. In…

High Energy Physics - Phenomenology · Physics 2017-12-13 Jun-Xia Zhang , Zhi-Gang Wang , Zun-Yan Di

We predict exotic doubly heavy--strange pentaquarks with minimal quark content $u\bar d sQQ'$ ($QQ'=cc,bc,bb$) within a coupled-channel unitary framework where the interaction is derived from an extension of the local hidden gauge approach…

High Energy Physics - Phenomenology · Physics 2026-05-26 Albert Feijoo , Eulogio Oset

The effect of quark-gluon vertex dressing on the ground state masses of the u/d-quark pseudoscalar, vector and axialvector mesons is considered with the Dyson-Schwinger equations. This extends the ladder-rainbow Bethe-Salpeter kernel to…

High Energy Physics - Phenomenology · Physics 2015-06-25 P. Watson , W. Cassing , P. C. Tandy

The masses of heavy tetraquarks with hidden charm and bottom are calculated in the framework of the relativistic quark model. The tetraquark is considered as the bound state of a heavy-light diquark and antidiquark. The light quark in a…

High Energy Physics - Phenomenology · Physics 2009-11-11 D. Ebert , R. N. Faustov , V. O. Galkin

A hadron's multiquark content reflects itself in the quark composition of the interpolator with which it has maximal overlap. The AdS/CFT dictionary translates the anomalous dimension of this interpolator into a mass correction for the…

High Energy Physics - Phenomenology · Physics 2015-05-27 Hilmar Forkel

We determine masses and decay constants of heavy-heavy and heavy-charm pseudoscalar mesons as a function of heavy quark mass using a fully relativistic formalism known as Highly Improved Staggered Quarks for the heavy quark. We are able to…

High Energy Physics - Lattice · Physics 2013-05-30 C. McNeile , C. T. H. Davies , E. Follana , K. Hornbostel , G. P. Lepage
‹ Prev 1 8 9 10 Next ›