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Related papers: Ground State Baryons in Covariant Level-Classifica…

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The essential points and physical backgrounds of the covariant level-classification scheme, recently proposed by us, are reviewed: In this scheme the general composite hadrons are classified as the multiplets with the U(12)SF * O(3,1)…

High Energy Physics - Phenomenology · Physics 2007-05-23 Shin Ishida , Muneyuki Ishida

The properties of ground-state baryons of light-quarks are investigated in U(12)-classification scheme of hadrons, recently proposed by us. In U(12), in addition to the ordinary 56 of SU(6)SF, the existence of the extra 56 with…

High Energy Physics - Phenomenology · Physics 2009-11-11 Muneyuki Ishida

The essential points and physical backgrounds of the covariant level-classification scheme, based on U(12)SF * O(3,1)L, are reviewed: This scheme is extended from the non-relativistic SU(6)SF * O(3)L scheme by introducing the new SU(2)-spin…

High Energy Physics - Phenomenology · Physics 2009-11-10 Muneyuki Ishida , Shin Ishida

Starting from the multi-local Klein-Gordon equations with Lorentz-scalar squared-mass operator we give a covariant quark representation of the general composite mesons and baryons with definite Lorentz transformation property. The…

High Energy Physics - Phenomenology · Physics 2008-11-26 Shin Ishida , Muneyuki Ishida

We examine possible assignments for known mesons to the predicted ground-state q bar q multiplets in the U~(12)_SF-classification scheme of hadrons, based on their observed properties. The masses of missing members of the ground-state…

High Energy Physics - Phenomenology · Physics 2007-05-23 Kenji Yamada

Starting from the multi-local Klein-Gordon equations with Lorentz-scalar squared-mass operator we give a covariant quark representation of the general composite mesons and baryons with definite Lorentz transformation property. The mass…

High Energy Physics - Phenomenology · Physics 2009-11-07 Shin Ishida , Muneyuki Ishida

We find possible candidates for the new type of q bar q meson, mesonic chiralons, whose existence is predicted in the covariant level-classification scheme of hadrons with U(12)_SF * O(3,1)_L symmetry, by assigning all the known…

High Energy Physics - Phenomenology · Physics 2007-05-23 Kenji Yamada

I classify exotic hadrons into two types, "genuine" and "hidden" exotics, and propose that the "hidden" exotics would be interpreted as "chiralons" in the ~U(12)_SF times O(3,1)_L-classification scheme of hadrons. Based upon this conjecture…

High Energy Physics - Phenomenology · Physics 2015-05-18 Kenji Yamada

It has recently been suggested that the parity doublet structure seen in the spectrum of highly excited baryons may be due to effective chiral restoration for these states. We argue how the idea of chiral symmetry restoration high in the…

High Energy Physics - Phenomenology · Physics 2009-11-07 T. D. Cohen , L. Ya. Glozman

Several years ago we have proposed a manifestly covariant $\tilde{U}(12)_{SF}$-classification scheme of hadrons, which maintains the successful $SU(6)_{SF}\otimes O(3)_{L}$ framework in Non-Relativistic Quark Model and is also reconcilable…

High Energy Physics - Phenomenology · Physics 2009-11-11 Shin Ishida

The narrow mesons, DsJ*(2317) and DsJ(2460), observed recently in the final states Ds+ pi0 and Ds*+ pi0 are pointed out to be naturally assigned as the ground-state scalar and axial-vector chiral states in the csbar system, which would…

High Energy Physics - Phenomenology · Physics 2007-05-23 Shin Ishida , Muneyuki Ishida , Tomohito Maeda , Masuho Oda , Kenji Yamada

We extend the chiral quark model for $u$, $d$, $c$ and $b$ quarks with vector mesons, which we proposed in the previous analysis, to a model with the $s$ quark. We include the nonet pseudo-scalar and vector mesons together with the singlet…

High Energy Physics - Phenomenology · Physics 2023-08-01 Bing-Ran He , Masayasu Harada , Bing-Song Zou

In order to classify the charmed-strange mesons, including puzzling D_{s0}^{*}(2317) and D_{s1}(2460), and recently observed D_{s1}^{*}(2710) and D_{sJ}^{*}(2860), we employ the U~(12)*O(3,1) level-classification scheme of hadrons proposed…

High Energy Physics - Phenomenology · Physics 2014-11-20 Tomohito Maeda , Kenji Yamada , Masuho Oda , Shin Ishida

The new narrow mesons observed recently in the final states Ds+ pi0 and Ds*+ pi0 are pointed out to be naturally assigned as the ground-state scalar and axial-vector chiralons in the c sbar system, which would newly appear in the covariant…

High Energy Physics - Phenomenology · Physics 2011-04-11 Shin Ishida , Muneyuki Ishida , Toshihiko Komada , Tomohito Maeda , Masuho Oda , Kenji Yamada , Ichiro Yamauchi

The electromagnetic decays of the ground state baryon multiplets with one heavy quark are calculated using Heavy Hadron Chiral Perturbation Theory. The M1 and E2 amplitudes for S^{*}--> S gamma, S^{*} --> T gamma and S --> T gamma are…

High Energy Physics - Phenomenology · Physics 2009-10-31 M. C. Banuls , A. Pich , I. Scimemi

The radiative transitions between ground-states (GS) of light q bar q mesons are investigated in the U~(12)-scheme. In this scheme the rich decay-spectra are offered even in transition between GS due to the appearance of chiral states. As a…

High Energy Physics - Phenomenology · Physics 2007-05-23 Tomohito Maeda , Kenji Yamada , Masuho Oda , Shin Ishida

We employ the chiral quark-soliton model and the heavy quark symmetry to describe spectra of charm and beauty baryons. Heavy baryons can be classified according to the SU(3) representations of the light sector. We argue that recently…

High Energy Physics - Phenomenology · Physics 2022-05-09 Maxim V. Polyakov , Michal Praszalowicz

We present a new classification scheme of baryon ground states and resonances into SU(3) flavor multiplets. The scheme is worked out along a covariant formalism with relativistic constituent quark models and it relies on detailed…

High Energy Physics - Phenomenology · Physics 2008-11-26 T. Melde , W. Plessas , B. Sengl

The gross features of the observed baryon excitation spectrum below 2 GeV are well explained if the spectrum generating algebra of its intrinsic orbital angular momentum states is o(4)*su(2)_I. The spins of the resonances are obtained…

High Energy Physics - Phenomenology · Physics 2009-10-30 M. Kirchbach

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…

Nuclear Theory · Physics 2011-07-19 Q. B. Li , P. N. Shen , Z. Y. Zhang , Y. W. Yu
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