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We propose a new model for describing baryon semi-leptonic decays for estimating $F$ and $D$ values with explicit breaking effects of both SU(3) and SU(2) flavor symmetry, where all possible SU(3) and SU(2) breaking effects are induced from…

High Energy Physics - Phenomenology · Physics 2008-11-26 T. Yamanishi

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

We study baryon excited states for quark confinement and chiral symmetry breaking. In the first part we discuss spatially deformed baryon excitations. As signals of deformation, we study masses and electromagnetic transitions. Such a study…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. Hosaka

We introduce diquarks as separable correlations in the two-quark Green's function to facilitate the description of baryons as relativistic three-quark bound states. These states then emerge as solutions of Bethe-Salpeter equations for…

High Energy Physics - Phenomenology · Physics 2008-11-26 S. Ahlig , R. Alkofer , C. Fischer , M. Oettel , H. Reinhardt , H. Weigel

Based on a contact lagrangian that incorporates the SU(3) flavor and SU(2) spin symmetries, we discuss the symmetry properties of the interactions among the heavy flavor meson-baryon $P_{\psi}^N$, $P_{\psi s}^\Lambda$ (with quark components…

High Energy Physics - Phenomenology · Physics 2024-04-08 Kan Chen , Bo Wang

It is argued that the baryon excitations group to four-dimensional partial waves described by means of the three Rarita-Schwinger (RS) fields [(\sigma -1 )/2 ,(\sigma -1)/2]* [(1/2, 0)+(0,1/2)] with \sigma =2,4 and 6, where all components…

High Energy Physics - Phenomenology · Physics 2007-05-23 M. Kirchbach

Being the fountainhead of transverse distortion and asymmetries in accordance to $``SSA=GPD \ast FSI\,"$, we study the spin flip generalized parton distribution. We demonstrate this transverse deformation by using the quark-scalar diquark…

High Energy Physics - Phenomenology · Physics 2024-09-27 Navpreet Kaur , Harleen Dahiya

We present first results for two-baryon correlation functions, computed using $N_f=2$ flavours of O($a$) improved Wilson quarks, with the aim of explaining potential dibaryon bound states, specifically the H-dibaryon. In particular, we use…

High Energy Physics - Lattice · Physics 2013-11-18 Anthony Francis , Chuan Miao , Thomas D. Rae , Hartmut Wittig

We have presented a pathway to map the internal structure of lowest-lying octet baryons by using one-loop quantum fluctuations of a fermion state in Yukawa theory. The structural interpretation of baryons carrying different amount of…

High Energy Physics - Phenomenology · Physics 2024-05-02 Navpreet Kaur , Harleen Dahiya

The S_3 symmetry corresponding to permuting the positions of the quarks within a baryon allows us to study the 70-plet of L=1 baryons without an explicit choice for the spatial part of the quark wave functions: given a set of operators with…

High Energy Physics - Phenomenology · Physics 2009-09-11 Hael Collins , Howard Georgi

In this work, we systematically investigate the dibaryons with charm number $C$=1 and strangeness number $S$=$\pm$ 1 from the interactions of a charmed baryon and a strange baryon $\Lambda_c\Lambda$, $\Lambda_c\Sigma^{(*)}$,…

High Energy Physics - Phenomenology · Physics 2023-01-04 Shu-Yi Kong , Jun-Tao Zhu , Jun He

We match the non-relativistic quark model, with both flavor dependent and flavor independent effective quark-quark interactions, to the spin-flavor operator basis of the 1/Nc expansion for the L=1 non-strange baryons. We obtain analytic…

Nuclear Theory · Physics 2016-02-10 Cintia Willemyns , Carlos Schat

By considering a flavour expansion about the SU(3)-flavour symmetric point, we investigate how flavour-blindness constrains octet baryon matrix elements after SU(3) is broken by the mass difference between quarks. Similarly to hadron masses…

High Energy Physics - Lattice · Physics 2020-01-08 J. M. Bickerton , R. Horsley , Y. Nakamura , H. Perlt , D. Pleiter , P. E. L. Rakow , G. Schierholz , H. Stüben , R. D. Young , J. M. Zanotti

A continuum approach to the three valence-quark bound-state problem in quantum field theory, employing parametrisations of the necessary kernel elements, is used to compute the spectrum and Poincar\'e-covariant wave functions for all…

Nuclear Theory · Physics 2019-09-18 Chen Chen , Gastao Krein , Craig D. Roberts , Sebastian M. Schmidt , Jorge Segovia

In this work, we investigate the decay behaviors of several higher strangeonia into $\Lambda\bar\Lambda$ through a hadronic loop mechanism, enabling us to predict some physical observables, including the branching ratios. Furthermore, we…

High Energy Physics - Phenomenology · Physics 2023-11-30 Zi-Yue Bai , Qin-Song Zhou , Xiang Liu

We present a unified framework for heavy tetraquark and pentaquark systems within the quark-diquark effective mass formalism, extending its baryon-calibrated construction to multiquark states without introducing sector-dependent parameters.…

High Energy Physics - Phenomenology · Physics 2026-03-06 Binesh Mohan , Rohit Dhir

Considering simultaneously isospin and SU(3) flavor symmetry breakings, we investigate the complete mass splittings of SU(3) baryons within a chiral soliton model, a {}"model-independent approach" being employed. In linear order several new…

High Energy Physics - Phenomenology · Physics 2012-09-03 Ghil-Seok Yang , Hyun-Chul Kim

We report an analysis of the impressive new lattice simulation results for octet baryon masses in 2+1-flavor QCD. The analysis is based on a low order expansion about the chiral SU(3) limit in which the symmetry breaking arises from terms…

High Energy Physics - Lattice · Physics 2010-04-06 R. D. Young , A. W. Thomas

The fine structure of the low energy part of the nucleon and strange hyperon spectra, which are formed of single states without parity doublets, may be understood in terms of an $SU(3)$ flavor-symmetric quark-quark interaction that…

High Energy Physics - Phenomenology · Physics 2011-04-20 L. Ya. Glozman , D. O. Riska

Using an SU(3) flavour symmetry breaking expansion in the quark mass, we determine the QCD component of the nucleon, Sigma and Xi mass splittings of the baryon octet due to up-down (and strange) quark mass differences in terms of the kaon…

High Energy Physics - Lattice · Physics 2013-05-30 R. Horsley , J. Najjar , Y. Nakamura , D. Pleiter , P. E. L. Rakow , G. Schierholz , J. M. Zanotti
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