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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 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

In the covariant level-classification scheme of hadrons based on U(12)SF * O(3,1)L symmetry, the ground state baryons and antibaryons are assigned to the (12 * 12 * 12)Sym = 364-multiplet in the spin-flavor U(12)SF symmetry. This multiplet…

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

The level classification of quark-antiquark systems is generally made by the LS-coupling scheme, resorting to the non-relativistic quark model. However, it has been well known that the pi-meson with the (L,S)=(0,0) shows also the properties…

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

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

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

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 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

Recently we have proposed a new level-classification scheme of hadrons with a manifestly covariant framework. In this scheme the requirement of chiral symmetry on the light quark leads to a prediction of existence of new type of scalars…

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

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

Starting from the bi-local Klein-Gordon Equation with spin-independent squared-mass operator, we give a covariant quark representation of general composite meson systems with definite Lorentz transformation properties. For benefit of this…

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

In the covariant level-classification scheme of hadrons proposed recently, the existence of "chiral particles", scalar and axial-vector mesons as the partners of the ground-state pseudo-scalar and vector mesons, respectively, were predicted…

High Energy Physics - Phenomenology · Physics 2007-05-23 Daiki Ito , Muneyuki Ishida , Shin Ishida , Toshihiko Komada , Hiroshi Tonooka , Kenji Yamada

In the covariant level-classification scheme of hadrons proposed recently, the existence of "chiral particles", scalar and axial-vector mesons as the partners of the ground-state pseudo-scalar and vector mesons, respectively, were predicted…

High Energy Physics - Phenomenology · Physics 2007-05-23 Daiki Ito , Muneyuki Ishida , Shin Ishida , Toshihiko Komada , Tomohito Maeda , Ichiro Yamauchi

We investigate the chiral mass splitting of parity-doubled J=0,1 states for c \bar{s} and c \bar{n} meson systems in the \tilde{U}(12)_{SF}-classification scheme of hadrons, using the linear sigma model to describe the light-quark…

High Energy Physics - Phenomenology · Physics 2015-06-25 Kenji Yamada , Tomohito Maeda , Shin Ishida

The extension of Non-Relativistic-to-Covariant classification scheme seems to be an urgent problem in the Hadron Spectroscopy. Here are given the recent results of our research. 1) Brief history of our way of the extension on Kinematical…

High Energy Physics - Phenomenology · Physics 2014-01-22 Shin Ishida

An extended chiral SU(3) model is applied to the description of dense, hot and strange hadronic matter. The degrees of freedom are the baryon octet and decuplet and the spin-0 and spin-1 meson multiplets. The parameters of the model are…

We point out that the spectrum of pseudoscalar and scalar mesons exhibits a cuasi-degenerate chiral nonet in the energy region around 1.4 GeV whose scalar component has a slightly inverted spectrum. Based on the empirical linear rising of…

High Energy Physics - Phenomenology · Physics 2008-11-26 Mauro Napsuciale , Simon Rodriguez

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
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