'Meson' presentation slideshows

The meson landscape

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Qiang Zhao Theory Division, Institute of High Energy Physics, CAS

Institute of High Energy Physics, CAS. Isospin violation and its correlation with OZI-evading process in quakonium hadronic decays. Qiang Zhao Theory Division, Institute of High Energy Physics, CAS. 1 st FCPPL Conference, Marseille, Jan. 14 - 18, 2008. Outline.

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QCD condensates and the behavior of mesons at finite density

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S=-2 hypernuclei predicted by ESC04 model

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Axial Vector Meson Emitting Decays of Bc

Axial Vector Meson Emitting Decays of Bc. Dated: 12 JUNE, 2012. VARIOUS QUARK LEVEL PROCESSES THAT CONTIBUTE TO THE NONLEPTONIC DECAYS. These Processes are Classified as:. FACTORIZATION SCHEME.

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THE PREDICTION OF LEPTONIC DECAY WIDTHS IN THE FRAME WORK OF CONSTITUENT QUARK MODELS

THE PREDICTION OF LEPTONIC DECAY WIDTHS IN THE FRAME WORK OF CONSTITUENT QUARK MODELS. BY DR. K.B. VIJAYA KUMAR READER,DEPARTMENT OF PHYSICS MANGALORE UNIVERSITY MANGALAGANGOTRI 574 199. AIM OF THE PROJECT.

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Dynamical coupled-channels s tudy of hadron r esonances and strangeness production

Dynamical coupled-channels s tudy of hadron r esonances and strangeness production. Hiroyuki Kamano (RCNP, Osaka U.) in collaboration with B. Julia-Diaz (Barcelona U.), T.-S. H. Lee (Argonne), A. Matsuyama (Shizuoka U.), S. Nakamura ( JLab ), T. Sato (Osaka U./KEK), N. Suzuki (Osaka U.).

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Covariant Density Functional Theory for Nuclei, Hypernulcei, and Neutron Stars

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Craig Roberts Physics Division

The Future of Hadron Physics. Craig Roberts Physics Division. Science Challenges for the coming decade: 2013-2022. Search for exotic hadrons Discovery would force dramatic reassessment of the distinction between the notions of matter fields and force fields

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Elliptic Flow in High Energetic Nuclear Collisions

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Standard Model

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Meson spectroscopy with unitary coupled-channels model

Meson spectroscopy with unitary coupled-channels model . Satoshi Nakamura Excited Baryon Analysis Center ( EBAC), JLab. Collaborators : H. Kamano (RCNP), T.-S.H. Lee (ANL), T. Sato (Osaka U). Why hadron spectroscopy ?. How. J PC , s pectrum, d ecay pattern key information

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FVTX Simulation and Analysis Software

FVTX Simulation and Analysis Software. Zhengyun You Los Alamos National Laboratory Nov-17-2010. Outline. Physics Motivation; Detector Performance; Charm / Beauty Separation (Blind Analysis); Verify DCA Distribution with Real Data; Di-muon Measurements Improvement;

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Open charm mesons in a hot and dense medium

Open charm mesons in a hot and dense medium. L. Tolos 1 , A. Ramos 2 and T. Mizutani 3 1 FIAS (University of Frankfurt) 2 Universitat de Barcelona 3 Virginia Polytechnic Institute and State University Phys. Rev. C77 (2008) 015207. Hadrons@FAIR, FIAS June 25-27, 2008

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CC2 Input Coupler Introduction, Installation, & Processing

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The Physics of high baryon densities

and not so high. The Physics of high baryon densities. Probing the QCD phase diagram The critical end point Properties of mesons in matter Baryon density vs. temperature Probing cold dense matter Conclusions. B. Friman, GSI. Critical endpoint. C o l o u r superconductor.

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? -meson Production in Heavy-Ion Collisions at RHIC

? -meson Production in Heavy-Ion Collisions at RHIC. Jin-Hui Chen Shanghai Institute of Applied Physics (SINAP), CAS. Outline Motivation of studying ? -meson Analysis details and technique Results and discussions Summary and Outlook.

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Low Mass Vector Meson at FAIR

Arun Prakash Banaras Hindu University. Low Mass Vector Meson at FAIR. Outline. Introduction Why to study Low Mass Vector Meson(LMVM) How to measure LMVM Past Experiments to detect them How we can Detect them in FAIR. Types of mesons. Type. S. L. P. J. J P. Example.

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