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Related papers: Constraints on widths of mixed pentaquark multiple…

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We discuss the constraints on the mass of the lighter top squark from \bbbar\ mixing in the minimal supersymmetric standard model. A light top squark whose mass is less than half of the $Z^0$-boson mass has not yet been excluded from direct…

High Energy Physics - Phenomenology · Physics 2008-11-26 G. C. Cho , Y. Kizukuri , N. Oshimo

A number of candidate multiquark hadrons, i.e., particle resonances with substructures that are more complex than the quark-antiquark mesons and three-quark baryons that are prescribed in the textbooks, have recently been observed. In this…

High Energy Physics - Experiment · Physics 2017-08-02 Stephen Lars Olsen

We develop quenched chiral perturbation theory for baryons using the graded-symmetry formalism of Bernard and Golterman and calculate non-analytic contributions to the baryon masses coming from quenched chiral loops. The usual term…

High Energy Physics - Lattice · Physics 2009-10-22 James N. Labrenz , Stephen R. Sharpe

The axial anomaly is responsible for the masses and mixing of the mesons $\eta$ and $\eta'$. An open question is if (and to what extent) it affects also other hadrons. We show that anomalous terms can be important to understand the…

High Energy Physics - Phenomenology · Physics 2017-12-14 Francesco Giacosa

A chiral effective theory of quarks and diquarks is formulated and applied to exotic tetraquarks and pentaquarks. The effective theory is similar to the chiral quark effective theory with the addition of diquark degrees of freedom and…

High Energy Physics - Phenomenology · Physics 2009-11-10 Deog Ki Hong , Young Jin Sohn , Ismail Zahed

We compute the spectra of exotic pentaquarks and monopole excitations of the low--lying ${1/2}^+$ and ${3/2}^+$ baryons in a chiral soliton model. Once the low--lying baryon properties are fit, the other states are predicted without any…

High Energy Physics - Phenomenology · Physics 2009-11-10 H. Weigel

We discuss the consequences of the chiral doubling scenario for baryons built of heavy and light quarks. In particular, we use the soliton description for baryons, demonstrating why each heavy-light baryon should be accompanied by the…

High Energy Physics - Phenomenology · Physics 2009-11-10 Maciej A. Nowak , Michal Praszalowicz , Mariusz Sadzikowski , Joanna Wasiluk

We critically examine the $\bar{K}N$ coupled-channel approach presented in [1] and demonstrate that it violates constraints imposed by chiral symmetry of QCD. The origin of this violation can be traced back to the off-shell treatment of the…

Nuclear Theory · Physics 2020-01-24 P. C. Bruns , A. Cieplý

We calculate the threshold $T$ matrices of the light pseudoscalar meson and heavy meson scattering to fourth order in heavy meson chiral perturbation theory. We determine the low-energy constants by fitting to the lattice QCD data points…

High Energy Physics - Phenomenology · Physics 2022-03-01 Bo-Lin Huang , Zi-Yang Lin , Shi-Lin Zhu

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

Using kaon secondary interactions in the material of the Belle detector, we search for both inclusive and exclusive production of the Theta(1540)+. We set an upper limit of 2.5% at the 90% C.L. on the ratio of the Theta(1540)+ to…

High Energy Physics - Experiment · Physics 2008-11-26 The Belle Collaboration , K. Abe

The $s-$wave meson-baryon scattering is analyzed for the strangeness S=0 sector in a Bethe-Salpeter coupled channel formalism incorporating Chiral Symmetry. Four channels have been considered: $\pi N$, $\eta N$, $K \Lambda$, $K \Sigma$. The…

High Energy Physics - Phenomenology · Physics 2009-11-07 Juan Nieves , Enrique Ruiz Arriola

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

In the Relativistic Mean Field Approximation three quarks in baryons from the lowest octet and the decuplet are bound by the self-consistent chiral field, and there are additional quark-antiquark pairs whose wave function also follows from…

High Energy Physics - Phenomenology · Physics 2010-11-19 Dmitri Diakonov , Victor Petrov

Inspired by the LHCb's discovery of hidden-charm pentaquarks, the anticharmed strange pentaquarks $P_{\bar c s}$ in a favor of the hadronic molecule picture are investigated from the one-boson-exchange model. Similar to the hidden-charm…

High Energy Physics - Phenomenology · Physics 2022-05-24 Nijiati Yalikun , Bing-Song Zou

The Weinberg compositeness criterion dictates that a pure shallow bound state is characterized by a large scattering length $a_0\gg\mathcal{O}(1/\beta)$ and a positive effective range $r_0$ that naturally scales to the size of…

High Energy Physics - Phenomenology · Physics 2025-03-10 Fang-Zheng Peng , Li-Sheng Geng , Ju-Jun Xie

Strangeness contents of baryons are calculated within rigid rotator model for arbitrary number of colors $N_c$. The problem of extrapolation to realistic value $N_c=3$ is noted, based on explicit calculations and comparison of rigid rotator…

High Energy Physics - Phenomenology · Physics 2009-11-11 Vladimir B. Kopeliovich , Andrei M. Shunderuk

The chiral partner structure of heavy baryons is studied using the bound state approach by binding the heavy-light mesons to nucleon as soliton in an effective Lagrangian for the pseudoscalar and vector mesons based on the hidden local…

High Energy Physics - Phenomenology · Physics 2013-04-02 Masayasu Harada , Yong-Liang Ma

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

In N = 1 super Yang-Mills theories, under certain conditions satisfied by the spectrum and the Yukawa couplings, the beta functions will vanish to all orders in perturbation theory. We address the generation of realistic quark mixing angles…

High Energy Physics - Phenomenology · Physics 2014-11-17 K. S. Babu , Ts. Enkhbat , I. Gogoladze