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.

Slides:



Advertisements
Similar presentations
HL-3 May 2006Kernfysica: quarks, nucleonen en kernen1 Outline lecture (HL-3) Structure of nuclei NN potential exchange force Terra incognita in nuclear.
Advertisements

The regularization dependence on the phase diagram in the Nambu-Jona-Lasinio model Hiroaki Kohyama (CYCU)
23 Jun. 2010Kenji Morita, GSI / XQCD20101 Mass shift of charmonium near QCD phase transition and its implication to relativistic heavy ion collisions Kenji.
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,
Su Houng Lee 1. Mesons with one heavy quark 2. Baryons with one heavy quark 3. Quarkonium Arguments based on two point function  can be generalized to.
1 Nuclear Binding and QCD ( with G. Chanfray) Magda Ericson, IPNL, Lyon SCADRON70 Lisbon February 2008.
Bottom-up AdS/QCD through a few examples Y. Kim (KIAS)
The structure of neutron star by using the quark-meson coupling model Heavy Ion Meeting ( ) C. Y. Ryu Soongsil University, Korea.
Nuclear Symmetry Energy from QCD Sum Rule Phys.Rev. C87 (2013) Recent progress in hadron physics -From hadrons to quark and gluon- Feb. 21, 2013.
Nuclear Symmetry Energy from QCD Sum Rule Heavy Ion Meeting , April 13, 2012 Kie Sang JEONG Su Houng LEE (Theoretical Nuclear and Hadron Physics.
New Frontiers in QCD, October 28th, 2011 Based on K. Kim, D. Jido, S.H. Lee PRC 84(2011) K. Kim, Y. Kim, S. Takeuchi, T. Tsukioka PTP 126(2011)735.
Relativistic chiral mean field model for nuclear physics (II) Hiroshi Toki Research Center for Nuclear Physics Osaka University.
Nuclear Symmetry Energy in QCD degree of freedom Phys. Rev. C87 (2013) (arXiv: ) Eur. Phys. J. A50 (2014) 16 Some preliminary results Heavy.
Isospin effect in asymmetric nuclear matter (with QHD II model) Kie sang JEONG.
Charm hadrons in nuclear medium S. Yasui (KEK) K. Sudoh (Nishogakusha Univ.) “Hadron in nucleus” 31 Nov. – 2 Dec arXiv:1308:0098 [hep-ph]
Enke Wang (Institute of Particle Physics, Huazhong Normal University) with A. Majumder, X.-N. Wang I. Introduction II.Quark Recombination and Parton Fragmentation.
In-medium hadrons and chiral symmetry G. Chanfray, IPN Lyon, IN2P3/CNRS, Université Lyon I The Physics of High Baryon Density IPHC Strasbourg, september.
Mass modification of heavy-light mesons in spin-isospin correlated matter Masayasu Harada (Nagoya Univ.) at Mini workshop on “Structure and production.
LBL 5/21/2007J.W. Holt1 Medium-modified NN interactions Jeremy W. Holt* Nuclear Theory Group State University of New York * with G.E. Brown, J.D. Holt,
In-Medium Studies of Omega, Nucleon and Open Charm with QCD Sum Rules Ronny Thomas Dresden, September 2007 Forschungszentrum Dresden-Rossendorf / TU Dresden.
XI th International Conference on Quark Confinement and the Hadron Petersburg, Russia Philipp Gubler (RIKEN, Nishina Center) Collaborator:
Nuclear Symmetry Energy in QCD degree of freedom Phys. Rev. C87 (2013) arXiv: Some preliminary results 2015 HaPhy-HIM Joint meeting Kie.
Pengfei Zhuang Physics Department, Tsinghua University, Beijing
Hadron to Quark Phase Transition in the Global Color Symmetry Model of QCD Yu-xin Liu Department of Physics, Peking University Collaborators: Guo H., Gao.
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,
Scalar response of the nucleon, Chiral symmetry and nuclear matter properties G. Chanfray, IPN Lyon, IN2P3/CNRS, Université Lyon 1 M. Ericson, IPN Lyon,
Role of vacuum in relativistic nuclear model A. Haga 1, H. Toki 2, S. Tamenaga 2 and Y. Horikawa 3 1. Nagoya Institute of Technology, Japan 2. RCNP Osaka.
Nuclear & Hadron Physics Group at Yonsei Univ. BNL 2003 Su Houng Lee, Yonsei Univ. P.Morath, S.Kim, SHL, W.Weise, PRL 82 (99) 3396 S. Kim, SHL, NPA 679.
Nuclear Symmetry Energy from QCD Sum Rule The 5 th APFB Problem in Physics, August 25, 2011 Kie Sang JEONG Su Houng LEE (Theoretical Nuclear and Hadron.
Interplay of antikaons with hyperons in nuclei and in neutron stars Interplay of antikaons with hyperons in nuclei and in neutron stars 13th International.
Nuclear Enthalpies J. Rozynek NCBJ Warszawa – arXiv nucl-th ( pedagogical example of volume/pressure corrections to EoS) ‘‘Is it possible to.
Modification of nucleon spectral function in the nuclear medium from QCD sum rules Collaborators: Philipp Gubler(ECT*), Makoto Oka Tokyo Institute of Technology.
Three-body force effect on the properties of asymmetric nuclear matter Wei Zuo Institute of Modern Physics, Lanzhou, China.
The phi meson in nuclear matter - recent result from theory - Talk at ECT* Workshop “New perspectives on Photons and Dileptons in Ultrarelativistic Heavy-Ion.
Korea-EU Alice 2004 Su Houng Lee Hungchong Kim, Taesoo Song, Yongjae Park, Yongshin Kwon (Osaka), Youngsoo Son, Kyungchul Han, Kyungil Kim Nuclear and.
1 Heavy quark system in vacuum and in medium Su Houng Lee In collaboration with Kenji Morita Also, thanks to group members: Present: T. Song, K.I. Kim,
Spectral functions of mesons at finite temperature/density Talk at the 31 st Reimei workshop on hadron physics in extreme conditions at J-PARC, Tokai,
And Mesons in Strange Hadronic Medium at Finite Temperature and Density Rahul Chhabra (Ph.D student) Department Of Physics NIT Jalandhar India In cooperation.
Helmholtz International Summer School, Dubna, 24 July 2008 Pion decay constant in Dense Skyrmion Matter Hee-Jung Lee ( Chungbuk Nat’l Univ.) Collaborators.
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,
1 Heavy quark system near Tc Su Houng Lee In collaboration with Kenji Morita Also, thanks to group members: Present: T. Song, K.I. Kim, W.S. Park, H. Park,
1 Properties of Quarkonia at T c Su Houng Lee In collaboration with Kenji Morita.
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.
Department of Physics, Sungkyunkwan University C. Y. Ryu, C. H. Hyun, and S. W. Hong Application of the Quark-meson coupling model to dense nuclear matter.
HADRON 2009, FloridaAnar Rustamov, GSI Darmstadt, Germany 1 Inclusive meson production at 3.5 GeV pp collisions with the HADES spectrometer Anar Rustamov.
Possible hadron physics To be done With use of unstable nuclei Teiji Kunihiro (Kyoto U.) Yonsei University, Korea.
Recent results from QCD sum rule analyses based on the maximum entropy method International Symposium on Chiral Symmetry in Hadrons and
Exact vector channel sum rules at finite temperature Talk at the ECT* workshop “Advances in transport and response properties of strongly interacting systems”
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:
Nuclear Symmetry Energy in QCD degree of freedom Phys. Rev
A novel probe of Chiral restoration in nuclear medium
Modifications of meson spectral functions in nuclear matter
CV (大西 明) 学部: 京都大学 ( ) 卒業研究: P4, Time-Reversal
QCD condensates and phi meson spectral moments in nuclear matter
Physics Opportunities with heavy quark system at FAIR
how is the mass of the nucleon generated?
Symmetry energy with non-nucleonic degrees of freedom
有限密度・ 温度におけるハドロンの性質の変化
Towards Understanding the In-medium φ Meson with Finite Momentum
The phi meson at finite density from a QCD sum rules + MEM approach
Scalar D mesons in nuclear matter
Present status of bottom up model: sample works
Hyun Kyu Lee Hanyang University
A possible approach to the CEP location
Nuclear Symmetry Energy and Compact Stars
The future of lattice studies in Korea
Theory on Hadrons in nuclear medium
Presentation transcript:

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 sum rules 1

2 Korea Rare Isotope Accelerator (KoRIA) Talk by B. Hong

3 Nuclear Symmetry Energy Shetty, Yennello, arXiv:

4 Nuclear Symmetry Energy Li, Chen, Ko, Phys. Rep. 464, 113 (08)

1. Few words on symmetry energy 5

6 QCD Energy Momentum Tensor Energy Density in asymmetric nuclear matter Linear density approximation

7 n p n p Nucleons in a background potential nucleons in the vacuum E p nucleons in the asymmetric matter

8 Medium modification Nucleon in Relativistic mean fields: (Di Toro et al) Hadrons in nuclear medium from QCD 1.Nucleons in symmetric nuclear matter: Cohen, Griegel, Furnstahl (91)  consistent with a strong scalar attraction and vector repulsion 2.Vector meson in medium: Hatsuda and Lee (92) : 4 quark condensate are important Symmetry Energy Average potential

9 QCD sum rules for Nucleon Small M 2 Large M 2 M 2

10 QCD sum rules for Nucleon in symmetric nuclear matter Cohen, Griegel, Furnstahl 92

11 QCD sum rules for Nucleon asymmetric nuclear matter K.S. Jeong, Lee 11

12  some detail  Expectation values

13 Results – Symmetry Energy

14 Results – Uncertainty

15 Results Important operator

16 Linear density approximation Condensate at finite density Operators in at finite density

17 1.An attempt to get some insight of Symmetry energy from QCD 2.Vector densities are important 3.Higher dimensional operators are important at higher density Summary