Collaborators: S. Sarkar, E.Oset and M. J. VicenteVacas

Slides:



Advertisements
Similar presentations
Exotic states in S=1 N  K system and low lying ½+ S=-1 resonances Kanchan Khemchandani, Departamento de Fisica, Universidad de Coimbra, Portugal. 19th.
Advertisements

Eightfold Way (old model)
Dynamically generated resonances from the vector octet-baryon decuplet interaction in the hidden gauge formalism Speaker: Bao-Xi Sun Institute of Theoretical.
EXOTIC MESONS WITH HIDDEN BOTTOM NEAR THRESHOLDS D2 S. OHKODA (RCNP) IN COLLABORATION WITH Y. YAMAGUCHI (RCNP) S. YASUI (KEK) K. SUDOH (NISHOGAKUSHA) A.
The Baryon octet-vector meson interaction and dynamically generated resonances in the S=0 sector Bao-Xi SUN ( 孙宝玺 ) Beijing University of Technology Hirschegg.
The Baryon octet-vector meson interaction and dynamically generated resonances in the S=0 sector 孙宝玺 北京工业大学 合作者 : 吕晓夫 四川大学 FHNP’15, 怀柔, 北京.
Munich, June 16th, 2010Exotic gifts of nature1 XIV International Conference on Hadron Spectroscopy J. Vijande University of Valencia (Spain) A. Valcarce,
Eightfold Way (old model)
Convergence of chiral effective theory for nucleon magnetic moments P. Wang, D. B. Leinweber, A. W. Thomas, A. G. Williams and R. Young.
Meson and Baryon Resonances from the interaction of vector mesons Hidden gauge formalism for vector mesons, pseudoscalars and photons Derivation of chiral.
Low energy scattering and charmonium radiative decay from lattice QCD
Symposium on the “12% rule” and “ puzzle”
Nρρ和Δρρ三强子束缚态的研究 孙宝玺 (北京工业大学) 陈华星 (北京航空航天大学) E. Oset(西班牙Valencia大学)
pp Annihilation _ Gluon- Rich Environment Direct resonant formation of states with all non-exotic quantum numbers. ⟹ excellent precision in mass.
The puzzle of (1405) and  (1475)
The study of pentaquark states in the unitary chiral approach
Institute of High Energy physics KEK, Hadron physics at J-PARC, Japan
Molecular Structures in Hidden Charm Meson and Charmed Baryon Spectrum
Polarization in charmless B VV decays
Three-body hadronic molecules.
from Belle, BaBar and CLEO
Search for exotic baryon resonances in pp collisions at the CERN SPS
Resonances in Ψˊ→π+π-π0 and study of Ψˊ→VP decays at BESII
An Effective operators analysis associated with the Higgs
Mesons, PANDA and the Importance of Scalar Glueball
E. Wang, J. J. Xie, E. Oset Zhengzhou University
Photoproduction of K* for the study of L(1405)
Nucleon Resonances from Lattice QCD
Quarks Þ strangeness Over the years inquiring minds have asked:
张仁友 (南昌, ) 中国科学技术大学粒子物理与技术中心
Possible Interpretations of DsJ(2632)
Exotic charmed four-quark mesons: molecules versus compact states
Observation of X(1835) in.
Baryon Resonances Baryon ground states and excited states
Guangxi Normal University
Testing the Structure of Scalar Mesons in B Weak Decays
Dibaryon production and structure
Excited State Spectroscopy from Lattice QCD
Decoding the riddle of Y(4260) and Zc(3900) Qiang Zhao
Dibaryons at CLAS Mikhail Bashkanov.
d*, a quark model perspective
Excited state nucleon spectrum
B physics at hadron collider
University of Minnesota on behalf of the CLEO Collaboration
Hidden charm spectroscopy from B-factories
有限密度・ 温度におけるハドロンの性質の変化
Recent Results of (2S) Decays at BESII
Study of excited baryons at BESII
Determination on F and D with SU(3) symmetry breaking effects and Δs distributions in the nucleon Teruya Yamanishi.
Search for (3770) non-DD-bar Decays
s, pentaquarks or excited heavy baryons, or both?
Coupled-channel effects in the decays of exotic states
Theoretical review of excited D*/Ds* mesons
Spectra and decays of hybrid charmonia
Pseudoscalar Quarkonium Exclusive Decays to Vector Meson Pair Cong-Feng Qiao Graduate.
Yong-Liang Ma In collaboration with M. Harada
Interpretation of the observed hybrid candidates by the QGC Model
Mixing of scalar meson and glueball
Recent Results of J/ and (2S) at BESII
Key issues about the nature of Y(4260)
Recent Results from Ψ(2S) and χcJ Decays
From J/ψ to LHCb Pentaquark ……and beyond
Understanding DsJ*(2317) and DsJ(2460)
Search for Lepton-number Violating Processes
New States Containing Charm at BABAR
Charmonium Group Meeting
School of Physical Science and Technology
AN EXPLANATION OF THE D5/2-(1930) AS A rD BOUND STATE
The decays KS, L into four leptons
Charmed Baryon Spectroscopy at BABAR
Presentation transcript:

Collaborators: S. Sarkar, E.Oset and M. J. VicenteVacas Dynamically generated resonances from the vector octet-baryon decuplet interaction in the hidden gauge formalism Speaker: Bao-Xi Sun Institute of Theoretical Physics, Beijing University of Technology Collaborators: S. Sarkar, E.Oset and M. J. VicenteVacas 2009.4.20 Nstar2009(Beijing)

1. Formalism 2. Results 3. Radiative decay

Vector-vector Interaction

Interaction Vertex

Anomalous Term

Anomalous Term

Bethe-Salpeter Eqution

Vector meson – baryon loop function in the dimensional regularization scheme

Vector meson-baryon loop function accounting for the width of the intermediate states

Decay modes

S=-1,I=0 Channel

S=-1,I=0 Channel

S=-1,I=1Channel

Resonance for S=-1,I=1 channel

0902.3150[hep-ph]

Radiative decay into γandΒD

Decay width for radiative decay

ρωφCouplings of resonances

Decay widths 0903.5138[hep-ph]

Conclusions Ten resonances in the different strangeness and isospin channels. Degenerate in JP=1/2-, 3/2-, 5/2-. Radiative widths are of the order of 1MeV. Radiative decay widths are different about one order of magnitude between the widths for different charge states of the same resonance.

Thanks