speaker: bao-xi sun institute of theoretical physics, beijing university of technology

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Dynamically generated resonances from the vector octet-baryon decuplet inter action in the hidden gauge formalism Speaker: Bao-Xi Sun Institute of Theoretical Physics, Beijin g University of Technology Collaborators: S. Sarkar, E.O set and M. J. VicenteVacas 2009.08.24 IWND2009(Shanghai)

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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 2009.08.24 IWND2009(Shanghai). - PowerPoint PPT Presentation

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Page 1: Speaker: Bao-Xi Sun Institute of Theoretical Physics, Beijing University of Technology

Dynamically generated resonances from the vector octet-baryon decuplet interaction in the hidden gaug

e formalism

Speaker: Bao-Xi SunInstitute of Theoretical Physics, Beijing University of Te

chnology

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

2009.08.24 IWND2009(Shanghai)

Page 2: Speaker: Bao-Xi Sun Institute of Theoretical Physics, Beijing University of Technology

1. Formalism

2. Results

3. Radiative decay

Page 3: Speaker: Bao-Xi Sun Institute of Theoretical Physics, Beijing University of Technology

Vector-vector Interaction

Page 4: Speaker: Bao-Xi Sun Institute of Theoretical Physics, Beijing University of Technology

Interaction Vertex

Page 5: Speaker: Bao-Xi Sun Institute of Theoretical Physics, Beijing University of Technology

Anomalous Term

Page 6: Speaker: Bao-Xi Sun Institute of Theoretical Physics, Beijing University of Technology

Anomalous Term

Page 7: Speaker: Bao-Xi Sun Institute of Theoretical Physics, Beijing University of Technology

Bethe-Salpeter Eqution

T V VGT

Page 8: Speaker: Bao-Xi Sun Institute of Theoretical Physics, Beijing University of Technology

Vector meson – baryon loop function in the dimensional regularization scheme

Page 9: Speaker: Bao-Xi Sun Institute of Theoretical Physics, Beijing University of Technology

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

Page 10: Speaker: Bao-Xi Sun Institute of Theoretical Physics, Beijing University of Technology

N

Page 11: Speaker: Bao-Xi Sun Institute of Theoretical Physics, Beijing University of Technology

Decay modes

Page 12: Speaker: Bao-Xi Sun Institute of Theoretical Physics, Beijing University of Technology

S=-1, I=0 Channel

Page 13: Speaker: Bao-Xi Sun Institute of Theoretical Physics, Beijing University of Technology

S=-1, I=0 Channel

Page 14: Speaker: Bao-Xi Sun Institute of Theoretical Physics, Beijing University of Technology

S=-1, I=1Channel

Page 15: Speaker: Bao-Xi Sun Institute of Theoretical Physics, Beijing University of Technology

Resonance for S=-1,I=1 channel

Page 16: Speaker: Bao-Xi Sun Institute of Theoretical Physics, Beijing University of Technology

0902.3150[hep-ph]

Page 17: Speaker: Bao-Xi Sun Institute of Theoretical Physics, Beijing University of Technology

Radiative decay into γandΒD

Page 18: Speaker: Bao-Xi Sun Institute of Theoretical Physics, Beijing University of Technology

Decay width for radiative decay

Page 19: Speaker: Bao-Xi Sun Institute of Theoretical Physics, Beijing University of Technology

ρωφCouplings of resonances

Page 20: Speaker: Bao-Xi Sun Institute of Theoretical Physics, Beijing University of Technology

Decay widths 0903.5138[hep-ph]

Page 21: Speaker: Bao-Xi Sun Institute of Theoretical Physics, Beijing University of Technology

Conclusions

1. Ten resonances in the different strangeness and isospin channels. Degenerate in JP=1/2-, 3/2-, 5/2-.

2. Radiative widths are of the order of 1MeV.

3. Radiative decay widths are different about one order of magnitude between the widths for different charge states of the same resonance.

Page 22: Speaker: Bao-Xi Sun Institute of Theoretical Physics, Beijing University of Technology

• Thanks