The future of lattice studies in Korea

Slides:



Advertisements
Similar presentations
Dubna, November 2003Joachim Stroth Hadron Structure in Dense Nuclear Matter Vector mesons Di-electron spectroscopy in heavy ion collisions The HADES spectrometer......
Advertisements

Denis Parganlija (Frankfurt U.) Meson 2010 Workshop, Kraków - Poland Structure of Scalar Mesons f 0 (600), a 0 (980), f 0 (1370) and a 0 (1450) Denis Parganlija.
Su Houng Lee Theme: 1.Will U A (1) symmetry breaking effects remain at high T/  2.Relation between Quark condensate and the ’ mass Ref: SHL, T. Hatsuda,
CERN-07 SHLee 1 Heavy Exotic Particle Production from HIC at LHC Su Houng Lee Yonsei Univ., Korea with Shigehiro Yasui, Wei Liu, Che-Ming Ko.
J. RuppertHot Quarks 2006, May 2006 What does the rho? Lessons from NA60's di-muon measurement. Jörg Ruppert Nuclear Theory, Department of Physics, Duke.
1 A Model Study on Meson Spectrum and Chiral Symmetry Transition Da
1 Chiral Symmetry Breaking and Restoration in QCD Da Huang Institute of Theoretical Physics, Chinese Academy of
Thermal phenomenological AdS/QCD 1. Thermal AdS/QCD 2. In-medium parameters 3. Chiral phase transition 4. Coupling constants Y. Kim (KIAS) with S.-J. Sin,
Hadrons and Nuclei : Introductory Remarks Lattice Summer School Martin Savage Summer 2007 University of Washington.
Has the critical temperature of the QCD phase transition been measured ?
1 Jozsó Zimányi (1931 – 2006). 2 Jozsó Zimányi I met Prof. Zimányi in India in Member, NA49 and PHENIX Collaborations Nuclear Equation of State.
1 Thermodynamics of two-flavor lattice QCD with an improved Wilson quark action at non-zero temperature and density Yu Maezawa (Univ. of Tokyo) In collaboration.
In-medium hadrons and chiral symmetry G. Chanfray, IPN Lyon, IN2P3/CNRS, Université Lyon I The Physics of High Baryon Density IPHC Strasbourg, september.
Su Houng Lee with Kie Sang Jeong 1. Few words on Nuclear Symmetry Energy 2. A QCD sum rule method 3. Preliminary results Nuclear Symmetry Energy from QCD.
XI th International Conference on Quark Confinement and the Hadron Petersburg, Russia Philipp Gubler (RIKEN, Nishina Center) Collaborator:
Su Houng Lee Theme: 1.Will U A (1) symmetry breaking effects remain at high T 2.Relation between Quark condensate and the ’ mass Ref: SHL, T. Hatsuda,
Chiral condensate in nuclear matter beyond linear density using chiral Ward identity S.Goda (Kyoto Univ.) D.Jido ( YITP ) 12th International Workshop on.
Su Houng Lee Quark condensate and the ’ mass  ‘ at finite temperature 1.
Su Houng Lee Theme: Relation between Quark condensate and the ’ mass Ref: SHL, T. Hatsuda, PRD 54, R1871 (1996) Y. Kwon, SHL, K. Morita, G. Wolf, PRD86,
Study of the QCD Phase Structure through High Energy Heavy Ion Collisions Bedanga Mohanty National Institute of Science Education and Research (NISER)
Istanbul 06 S.H.Lee 1 1.Introduction on sQGP and Bag model 2.Gluon condensates in sQGP and in vacuum 3.J/  suppression in RHIC 4.Pertubative QCD approach.
Eigo Shintani (KEK) (JLQCD Collaboration) KEKPH0712, Dec. 12, 2007.
Denis Parganlija, A Linear Sigma Model with Vector Mesons and Global Chiral Invariance Denis Parganlija In collaboration with Francesco Giacosa,
Masayasu Harada (Nagoya Univ.) based on (mainly) M.H. and K.Yamawaki, Phys. Rev. Lett. 86, 757 (2001) M.H. and C.Sasaki, Phys. Lett. B 537, 280 (2002)
Korea-EU Alice 2004 Su Houng Lee Hungchong Kim, Taesoo Song, Yongjae Park, Yongshin Kwon (Osaka), Youngsoo Son, Kyungchul Han, Kyungil Kim Nuclear and.
A chiral model for low-energy hadrons Francesco Giacosa In collaboration with Achim Heinz, Stefan Strüber, Susanna Gallas, Denis Parganlija and Dirk Rischke.
Quark spectrum near chiral and color-superconducting phase transitions Masakiyo Kitazawa Kyoto Univ. M.K., T.Koide, T.Kunihiro and Y.Nemoto, PRD70,
Time Dependent Quark Masses and Big Bang Nucleosynthesis Myung-Ki Cheoun, G. Mathews, T. Kajino, M. Kusagabe Soongsil University, Korea Asian Pacific Few.
Denis Parganlija (Frankfurt U.) Excited QCD 2010, Tatranska Lomnica/Slovakia Nature of Light Scalar Mesons f 0 (600), a 0 (980), f 0 (1370) and a 0 (1450)
? composite ? H. Fritzsch LMU Munich.
XXXI Bienal de la RSEF, Granada, España, septiembre Angel Gómez Nicola Universidad Complutense Madrid COEFICIENTES DE TRANSPORTE EN UN GAS.
Cosmological constant Einstein (1917) Universe baryons “Higgs” condensate Englert-Brout, Higgs (1964) bare quark 3 “Chiral” condensate Nambu (1960)
1 Meson mass in nuclear medium Su Houng Lee Thanks to: Hatsuda + former collaborators + and to Kenji Morita(GSI) and Taesoo Song(A&M) 1.Phase transition,
QM06 - S.H.Lee 1 1.Comments on J/  dissociation by partons 2.Progress in QCD calculations: LO and NLO 3. Dissociation due to thermal gluons and quarks.
Toru T. Takahashi with Teiji Kunihiro ・ Why N*(1535)? ・ Lattice QCD calculation ・ Result TexPoint fonts used in EMF. Read the TexPoint manual before you.
Proton Mass and EoS for Compressed Baryonic Matter ATHIC 14/11/12 Mannque Rho (Saclay and Hanyang)
1 Keitaro Nagata and Atsushi Hosaka Research Center for Nuclear Physics, Osaka Univ. Quark-Diquark approach for the nucleon and Roper resonance Workshop.
Beijing, QNP091 Matthias F.M. Lutz (GSI) and Madeleine Soyeur (Saclay) Irfu/SPhN CEA/ Saclay Irfu/SPhN CEA/ Saclay Dynamics of strong and radiative decays.
Nuclear Matter Density Dependence of Nucleon Radius and Mass and Quark Condensates in the GCM of QCD Yu-xin Liu Department of Physics, Peking University.
Denis Parganlija (Vienna UT) Mesons in non-perturbative and perturbative regions of QCD Mesons in non-perturbative and perturbative regions of QCD Denis.
高密度クォーク物質における カイラル凝縮とカラー超伝導の競 合 M. Kitazawa,T. Koide,Y. Nemoto and T.K. Prog. of Theor. Phys., 108, 929(2002) 国広 悌二 ( 京大基研) 東大特別講義 2005 年 12 月 5-7 日 Ref.
Denis Parganlija (Frankfurt U.) Finite-Temperature QCD Workshop, IST Lisbon Non-Strange and Strange Scalar Quarkonia Denis Parganlija In collaboration.
Su Houng Lee 1. Few words on a recent sum rule result 2. A simple constituent quark model for D meson 3. Consequences 4. Summary D meson in nuclear medium:
C.A. Dominguez Centre for Theoretical Physics & Astrophysics University of Cape Town Department of Physics, Stellenbosch University South Africa XII WORKSHOP.
Dilepton and the QCD CP What is the QCD CP Dileptons.
-Nucleon Interaction and Nucleon Mass in Dense Baryonic Matter
Institute of High Energy physics KEK, Hadron physics at J-PARC, Japan
Exotic mesons in holographic QCD
QCD with chiral chemical potential: models versus lattice
A novel probe of Chiral restoration in nuclear medium
mesons as probes to explore the chiral symmetry in nuclear matter
Extending the Linear Sigma Model to Nf = 3
co-authors B. Kaempfer (HZDR, Germany), L.P. Kaptari (BLTPh)
Scalar Meson σ(600) in the QCD Sum Rule
Strangeness and charm in hadrons and dense matter, YITP, May 15, 2017
Physics Opportunities with heavy quark system at FAIR
p p interaction in nuclear matter
The Operator Product Expansion Beyond Perturbation Theory in QCD
Chiral Structure of Hadronic Currents
Towards Understanding the In-medium φ Meson with Finite Momentum
QCD and Heavy-ion Collisions
The phi meson at finite density from a QCD sum rules + MEM approach
Scalar D mesons in nuclear matter
QCD和則とMEMを用いた有限密度中のvector mesonの研究の現状と最近の発展
Infrared Slavery Above and Hadronic Freedom Below Tc
Present status of bottom up model: sample works
Composite Weak Bosons LHC.
Hyun Kyu Lee Hanyang University
Dilaton in Baryonic Matter
Theory on Hadrons in nuclear medium
Presentation transcript:

The future of lattice studies in Korea Few examples: Low energy collision code comparison group. Heavy quark working group Korean lattice group Website for sharing codes usage Suggestion web

Brain storming  Many previous work Soft modes, scalar meson: Hatsuda, Kunihiro (85,87) Pseudoscalar mesons: Bernard, Jaffe, Meissner (88), Klimt, Lutz, Vogel, Weise (90) Brown-Rho: 91 4. Vector mesons: Hatsuda, Lee (92) …..

Summary Chiral symmetry: Experience taught us to measure small width particles G<100 MeV Theory tells us to look at chiral partners K* K1 are chiral partners could be done at J-PARC !! And possibly at other facilities  can link chiral symmetry restoration to mass generation in hadrons

Future of lattice QCD in Korea : I want to try K*, K1 at finite T on the lattice T dependence of Higher gluon operators : Gradient flow ? Test ……?