'Chiral symmetry' diaporamas de présentation

????? 12 ??????????

????? 12 ??????????. ??????????????????????????????????????????????? ????????????????????? ???????????????? ??????????????????????????? ??????????????????????????????????????? ????????????????????????????????. ??????????????????????????????

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Quark deconfinement and symmetry

Quark deconfinement and symmetry. Hiroaki Kouno Dept. of Phys., Saga Univ. Collaboration with K. Kashiwa, Y. Sakai, M. Yahiro ?? Kyushu. Univ.) and M. Matsuzaki (Fukuoka Univ. of Education). Confinement of quark.

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Update on Search for Chiral Symmetry Restoration in Heavy-Ion Collisions

Update on Search for Chiral Symmetry Restoration in Heavy-Ion Collisions. Ralf Rapp Cyclotron Institute + Dept of Phys & Astro Texas A&M University College Station, USA Heavy-Ion Forum Seminar CERN (Geneva, Switzerland), 03.05.12.

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? D ??????????????

? D ??????????????. arXiv:1308.0098 [ hep -ph]. ????? (KEK). ????? ????? ( ?????? ). KEK ???? ????????????????? = ????? = ? @ 5-6 Aug . 2013. Contents. 1. Introduction to charm ( bottom ) nuclei 2 . Heavy h adron mass and gluon field

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??????????????? ?????? ????. 23.11.11

O .?. ?????? ????, ????. ??????????????? ?????? ????. 23.11.11. Outline. When strange quarks can be heavy: multiscale hadrons (Squared) Nucleon mass >> strange mass >> (intrinsic) higher twist scale Strangeness polarization

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Recent RHIC Results with AA Mark D. Baker Brookhaven National Laboratory

Recent RHIC Results with AA Mark D. Baker Brookhaven National Laboratory. The Motivation What have we learned about AA? What have we learned about QCD? Conclusions. Many thanks to: Peter Steinberg. The RHIC community .

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Chiral Symmetry Breaking and Restoration and Consistent Meson Spectrum

Chiral Symmetry Breaking and Restoration and Consistent Meson Spectrum. Da Huang Institute of Theoretical Physics, Chinese Academy of Sciences @CPOD, Wuhan. Content. Dynamically Generated Spontaneous Chiral Symmetry Breaking In Chiral Dynamical Model At Zero Temperature

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Dileptons at RHIC

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Studying medium modifications of mesons in elementary reactions

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PANDA: Experiments to Study the Properties of Charm in Dense Hadronic Matter

PANDA: Experiments to Study the Properties of Charm in Dense Hadronic Matter. Overview of the PANDA Pbar-A Program The Pbar Facility The PANDA Detector Selected Simulation Results. Why Are Hadrons So Heavy?. Hadron Masses. 2M u + M d ~ 15 MeV/c 2 M p = 938 MeV/c 2.

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SOME RELEVANT PUBLICATIONS:

SOME RELEVANT PUBLICATIONS: Homogeneous Solution Lattice Model [E = experiment, T = theory] 1. F.C. Frank, "On Spontaneous Asymmetric Synthesis", Biochim.

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Hidden Local Symmetry as an Effective Field Theory of QCD

Hidden Local Symmetry as an Effective Field Theory of QCD. Masayasu Harada (Nagoya Univ.). @ KIAS-Hanyang Joint Workshop on Multifaceted Skyrmions and Effective Field Theory (October 26, 2004 KIAS). based on M.H. and K.Yamawaki, Phys. Rept. 381, 1 (2003)

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Chiral symmetry breaking and low energy effective nuclear Lagrangian

Chiral symmetry breaking and low energy effective nuclear Lagrangian. Eduardo A. Coello Perez. QCD Lagrangian. The quantum chromodynamics Lagrangian is given by If the mass of the quarks is neglected, the Lagrangian takes the form. Right and left components.

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Lifetime measurements in 128 Cs and 132 La as a test of chirality

Lifetime measurements in 128 Cs and 132 La as a test of chirality. Julian Srebrny Nuclear Physics Division Institute of Experimental Physics Warsaw University. Kazimierz Dolny September 2005. Three angular momentum vectors can form two systems of different handedness.

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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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Alex Kalloniatis (CSSM, Adelaide) & Sergei N. Nedelko (JINR, Dubna)

CHIRALITY IN A DOMAIN MODEL FOR THE QCD VACUUM. Alex Kalloniatis (CSSM, Adelaide) & Sergei N. Nedelko (JINR, Dubna). QCD@Work, Conversano, June 14-18, 2003. Singular Fields in the QCD Partition Function. In general, action will be infinite . exp(-action)=0.

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Conductivity and non-commutative holographic QCD

Conductivity and non-commutative holographic QCD. M. Ali- Akbari School of physics, IPM, Iran Sixth Crete regional meeting in string theory Milos , 2011. Outline. Conductivity from AdS /CFT Sakai-Sugimoto model 2-1. Low temperature

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f meson production in =200 GeV proton+proton collisions at PHENIX

f meson production in =200 GeV proton+proton collisions at PHENIX. ?? ?? Yuji Tsuchimoto tsuchimoto@bnl.gov High-energy Hadron Physics group, Department of Physics, Hiroshima University, Japan. Why am I interested in f ?. Chiral symmetry Lagrangean in the Normal QCD Vacuum

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Quantum Hall transition in graphene with

Quantum Hall transition in graphene with correlated bond disorder. -- Unconventional Hall transition at n=0 Landau level --. T. Kawarabayshi (Toho University) Y. Hatsugai (University of Tsukuba) H. Aoki (University of Tokyo) ArXiv:0904.1927.

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Particles and Forces

Particles and Forces. Bosons. Chiral . For m=0 the helicity and the chirality are the same. The form of the spinor for m=0 maintains the strict relationship between the spin direction and the action of the gamma-5 matrix. In the limit of quark mass ?0 there is a chiral symmetry for quarks.

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