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Related papers: Pentaquark decay is suppressed by chirality conser…

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We investigate the hidden-charm pentaquarks as superpositions of $\Lambda_c \bar{D}^{(*)}$ and $\Sigma_c^{(*)} \bar{D}^{(*)}$ (isospin $I = 1/2$) meson-baryon channels coupled to a $uudc\bar{c}$ compact core by employing an interaction…

It is pointed out that the previously suggested interpretation of the hidden-charm pentaquarks $P_c(4312)$, $P_c(4440)$ and $P_c(4457)$ as molecular bound states of $\Sigma_c \bar D$ and $\Sigma_c \bar D^*$ baryon-meson pairs gives rise to…

High Energy Physics - Phenomenology · Physics 2019-08-28 M. B. Voloshin

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 consider hidden charm pentaquarks as hadroquarkonium states in a QCD inspired approach. Pentaquarks arise naturally as bound states of quarkonia excitations and ordinary baryons. The LHCb $P_c(4450)$ pentaquark is interpreted as a…

High Energy Physics - Phenomenology · Physics 2018-02-14 Michael I. Eides , Victor Yu. Petrov , Maxim V. Polyakov

A systematic lowering in mass of strangeness ambiguous $pK^0_S$ peaks relative to the $nK^+$ is noted. We discuss how measurement of $\gamma p\to \Theta^+ K^0_S\to p K^0_S K^0_S \to p\pi^+\pi^-\pi^+\pi^-$ in association with $\gamma p\to…

High Energy Physics - Phenomenology · Physics 2009-11-10 Qiang Zhao , Frank E. Close

With a sample of 232x10^6 Upsilon(4S) --> BBbar events collected with the BaBar detector, we study the decay B+ --> p pbar K+ excluding charmonium decays to ppbar. We measure a branching fraction Br(B+ --> p pbar…

High Energy Physics - Experiment · Physics 2010-03-19 B. Aubert , BABAR Collaboration

Recent experimental evidence for the Theta^+(1540) has given rise to much theoretical interest in exotic baryons. The Theta^+ is a baryon that has strangeness S=+1, meaning that it contains an anti-strange quark. Thus it cannot be…

High Energy Physics - Phenomenology · Physics 2007-05-23 Margaret E Wessling

Hidden-charm pentaquarks are analysed in Group Theory in the baryon-meson molecule picture within the framework of the constituent quark model. The investigation of strong decays of pentaquark resonances reveals that pentaquark states of…

High Energy Physics - Phenomenology · Physics 2023-04-11 Kanokphon Phumphan , Kai Xu , Wiriya Ruangyoo , Chia-Chu Chen , Ayut Limphirat , Yupeng Yan

We study the multiquark hadrons in large $N$ QCD under the 't-Hooft limit, extending Witten's picture of the baryons. We explore the decay widths of tetraquarks, pentaquarks and dibaryons. Based on the decay behaviors, we point out in the…

High Energy Physics - Phenomenology · Physics 2018-12-18 Luciano Maiani , Veronica Riquer , Wei Wang

We study the pentaquark $uudd\bar s$ with $J=3/2$ and I=1 ($\Theta^{++}$) in the QCD sum rule approach. We derive the QCD sum rules for positive and negative parity states of the pentaquark. The QCD sum rule predicts that there exists…

High Energy Physics - Phenomenology · Physics 2009-11-10 Tetsuo Nishikawa , Yoshiko Kanada-En'yo , Osamu Morimatsu , Yoshihiko Kondo

If a narrow Theta^+ pentaquark exists, it is likely that a ud\bar s-ud triquark-diquark configuration is a significant component of its wave function. If so, the mechanism responsible for the binding of a triquark and a diquark is also…

High Energy Physics - Phenomenology · Physics 2010-04-05 Marek Karliner , Harry J. Lipkin

By assuming SU(6)_cs symmetry for pentaquark decays one finds a selection rule, which strongly reduces the number of states able to decay into a baryon and a meson final state and allows an intriguing identification for the Theta^+ particle…

High Energy Physics - Phenomenology · Physics 2010-11-05 F. Buccella

The data on the reactions K^+Xe --> K^0 \gamma X and K^+Xe --> K^+ \gamma X, obtained with the bubble chamber DIANA, have been analyzed for possible radiative decays of the \Theta^+(1540) baryon: \Theta^+ --> K^0 p \gamma and \Theta^+ -->…

If the Theta^+(1540) is interpreted as a bound state of a $\bar s$ quark and two (ud) diquarks in a relative P-wave, then it is very likely that there exist pentaquark states with a heavy antiquark, $\bar b$ or $\bar c$, and two ``light''…

High Energy Physics - Phenomenology · Physics 2010-04-05 Iain W. Stewart , Margaret E. Wessling , Mark B. Wise

Based on SU(3) flavor symmetry, we decompose the decay amplitudes of bottom baryon decays to a pseudoscalar meson and an octet (a decuplet) pentaquark in terms of three (two) invariant amplitudes $T_1$ and $T_{2,3}$ ($\tilde T_1$ and…

High Energy Physics - Phenomenology · Physics 2015-12-02 Hai-Yang Cheng , Chun-Khiang Chua

We investigate the effect of chiral phase transition on the pentaquark $\Theta^+$ mass and width at one-loop level of $N\Theta^+K$ coupling at finite temperature and density. The behavior of the mass, especially the width in hadronic medium…

Nuclear Theory · Physics 2009-11-10 Xuguang Huang , Xuewen Hao , Pengfei Zhuang

Recently the so-called $\Theta^+$ resonance has been reported first from SPring8\cite{nakano} and many following experiments showed apparent confirmation of the state. Since $\Theta^+$ exclusively decays into either $K^+ n$ or $K^0 p$, it…

High Energy Physics - Experiment · Physics 2009-11-10 Tadafumi Kishimoto , Toru Sato

We propose a collective stringlike model of pentaquarks with the geometry of an equilateral tetrahedron in which the four quarks are located at the four corners and the antiquark in its center. The nonplanar equilibrium configuration is a…

High Energy Physics - Phenomenology · Physics 2017-11-02 R. Bijker , M. M. Giannini , E. Santopinto

$\Theta^+$ is a putative light pentaquark state of positive parity with minimal quark content $(uudd\bar{s})$. It naturally emerges in chiral models for baryons, but experimental evidence is uncertain. We review the theoretical foundations…

High Energy Physics - Phenomenology · Physics 2025-08-22 Michal Praszalowicz