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相关论文: The S- and P-wave low-lying baryons in the chiral …

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It is shown from rigorous three-body Faddeev calculations that the masses of all 14 lowest states in the $N$ and $\Delta$ spectra can be described within a constituent quark model with a Goldstone-boson-exchange interaction plus linear…

高能物理 - 唯象学 · 物理学 2009-10-28 L. Ya. Glozman , Z. Papp , W. Plessas

The orbitally excited heavy quark baryons are studied in the Callan Klebanov bound state model with heavy spin symmetry. First, a compact description of the large $N_c$, infinite heavy quark mass bound state wavefunctions and the collective…

高能物理 - 唯象学 · 物理学 2010-11-01 Joseph Schechter , Anand Subbaraman

In the framework of the SU(3) chiral quark model, the $S-$wave baryon-baryon bound states are investigated. It is found that according to the symmetry character of the system and the contributions from chiral fields, there are three types…

核理论 · 物理学 2009-11-06 P. N. Shen , Q. B. Li , Z. Y. Zhang , Y. W. Yu

We study heavy-light baryon resonances with quantum numbers J^P=1/2^- in terms of the non-linear chiral SU(3) Lagrangian. Within the chi-BS(3) approach a parameter-free leading order prediction is obtained for the scattering of Goldstone…

高能物理 - 唯象学 · 物理学 2010-12-16 M. F. M. Lutz , E. E. Kolomeitsev

Single pion transitions of S wave to S wave, P wave to S wave and P wave to P wave heavy baryons are analyzed in the framework of the Heavy Quark Symmetry limit (HQS). We use a constituent quark model picture for the light diquark system…

高能物理 - 唯象学 · 物理学 2009-10-31 F. Hussain , J. G. Koerner , Salam Tawfiq

The low-lying $S$-wave $QQ\bar{s}\bar{s}$ ($Q=c, b$) tetraquark states with $IJ^P=00^+$, $01^+$ and $02^+$ are systematically investigated in the framework of complex scaling range of chiral quark model. Every structure including…

高能物理 - 唯象学 · 物理学 2020-09-30 Gang Yang , Jialun Ping , Jorge Segovia

Mesonic fluctuations around the chiral solitons are investigated in the SU(3) chiral quark soliton model. Since the soliton takes the non-hedgehog shape for the hyperons and the hedgehog one for the non-hedgehog baryons in our approach, the…

高能物理 - 唯象学 · 物理学 2007-05-23 Satoru Akiyama , Yasuhiko Futami

Inspired by the resonance $T_{cc}^+(3875)$ recently observed by the LHCb Collaboration, we systematically explore the $S$- and $P$-wave $cc\bar{q}\bar{q}'$ $(\bar{q},\bar{q}' = \bar{u}, \bar{d}, \bar{s})$ systems in a chiral SU(3) quark…

高能物理 - 唯象学 · 物理学 2024-03-25 Du Wang , Ke-Rang Song , Wen-Ling Wang , Fei Huang

In this work, we study the $T\bar{T}$-type molecular systems systematically via one pion exchange model, where $T$ denotes the narrow $J^P=1^+$ $D_1$ meson or $2^+$ $D_2^*$ meson and $\bar{T}$ is its antiparticle. With the effective…

高能物理 - 唯象学 · 物理学 2016-06-15 Rui Chen , Xiang Liu , Yan-Rui Liu , Shi-Lin Zhu

A constituent quark model, which has recently been successfully applied to the study of heavy quarkonium properties such as its spectrum but also a diverse array of observables related with their electromagnetic, strong and weak decays and…

高能物理 - 唯象学 · 物理学 2020-03-04 Gang Yang , Jialun Ping , Pablo G. Ortega , Jorge Segovia

The non-strange baryon spectrum is studied within a three-body model that incorporates relativistic kinematics. We found that the combined effect of relativistic kinematics together with the pion exchange between quarks is able to reverse…

高能物理 - 唯象学 · 物理学 2009-11-10 H. Garcilazo , A. Valcarce

The possible candidates of $S-$wave dibaryons with various strange numbers are studied under the chiral SU(3) quark model. It is shown that there are three types of baryon-baryon bound states. The states of the first type are called…

核理论 · 物理学 2011-07-19 Q. B. Li , P. N. Shen , Z. Y. Zhang , Y. W. Yu

The possibility of $QQ\bar{q}\bar{q}$ heavy-light four-quark bound states has been analyzed by means of the chiral SU(3) quark model, where $Q$ is the heavy quark ($c$ or $b$) and $q$ is the light quark ($u$, $d$ or $s$). We obtain a bound…

核理论 · 物理学 2008-11-26 M. Zhang , H. X. Zhang , Z. Y. Zhang

A calculational scheme is developed to evaluate chiral corrections to properties of composite baryons with composite pions. The composite baryons and pions are bound states derived from a microscopic chiral quark model. The model is…

高能物理 - 唯象学 · 物理学 2009-11-07 P. J. A. Bicudo , G. Krein , J. E. F. T. Ribeiro

The use of Heavy Quark Symmetry to study bottom and charmed baryons leads to important simplifications of the non-relativistic three body problem, which turns out to be easily solved by a simple variational ansatz. Our simple scheme…

核理论 · 物理学 2009-09-29 C. Albertus , J. E. Amaro , E. Hernandez , J. Nieves

The structures of $N\Omega_{(2,1/2)}$ and $\Delta\Omega_{(3,3/2)}$ with strangeness $s=-3$ are dynamically studied in both the chiral SU(3) quark model and the extended chiral SU(3) quark model by solving a resonating group method (RGM)…

核理论 · 物理学 2007-05-23 Dai Lian-Rong , Zhang Dan , Li Chun-Ran , Tong Lei

During the last decades, numerous exotic states which cannot be explained by the conventional quark model have been observed in experiment. Some of them can be understood as two-body hadronic molecules, such as the famous $X(3872)$,…

高能物理 - 唯象学 · 物理学 2019-08-07 Li Ma , Qian Wang , Ulf-G. Meißner

We study the strong interactions of the L=1 orbitally excited baryons with one heavy quark in the framework of the Heavy Hadron Chiral Perturbation Theory. To leading order in the heavy mass expansion, the interaction Lagrangian describing…

高能物理 - 唯象学 · 物理学 2014-11-17 Dan Pirjol , Tung-Mow Yan

The lower excitation spectrum of the nucleon and $\Delta$ is calculated in a relativistic chiral quark model. Contributions of the second order self-energy and exchange diagrams due-to pion fields to the mass spectrum of the SU(2) baryons…

高能物理 - 唯象学 · 物理学 2009-11-10 E. M. Tursunov

Beyond the scale of spontaneous breaking of chiral symmetry light and strange baryons should be considered as systems of three constituent quarks with confining interaction and a chiral interaction that is mediated by Goldstone bosons…

高能物理 - 唯象学 · 物理学 2009-10-30 L. Ya. Glozman
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