Nuclear Symmetry Energy in holographic QCD

Slides:



Advertisements
Similar presentations
1 Holographic description of Hadrons from String Theory Shigeki Sugimoto (IPMU) Rencontres de Moriond, March 25, La Thuile, Italy (based on works.
Advertisements

Analysis of QCD via Supergravity S. Sugimoto (YITP) based on hep-th/ (T. Ibaraki + S.S.) Windows to new paradigm in particle Sendai.
Spectroscopy of fermionic operators in AdS/CFT with flavor Ingo Kirsch Workshop „QCD and String Theory“ Ringberg Castle, Tegernsee, July 2-8, 2006 I. K.,
Brane-World Inflation
With Y. Seo, J.P. Shock, D. Zoakos(0911.xxxx) CY.Park, KH. Jo, BH Lee( )
Precision Holographic Baryons PILJIN YI (KIAS) Baryons 2010, Osaka, December 2010 Koji Hashimoto Deog-Ki Hong Norihiro Iizuka Youngman Kim Sangmin Lee.
Topological current effect on hQCD at finite density and magnetic field Pablo A. Morales Work in collaboration with Kenji Fukushima Based on Phys. Rev.
23 Jun. 2010Kenji Morita, GSI / XQCD20101 Mass shift of charmonium near QCD phase transition and its implication to relativistic heavy ion collisions Kenji.
Baryon Chemical Potential in AdS/CFT Shin Nakamura CQUeST and Hanyang Univ. Refs. S.N.-Seo-Sin-Yogendran, hep-th/ and arXiv: (hep-th)
Gauge/Gravity Duality 2 Prof Nick Evans AdS/CFT Correspondence TODAY Quarks Deforming AdS Confinement Chiral Symmetry Breaking LATER Other brane games.
3rd International Workshop On High Energy Physics In The LHC Era.
Gauge/Gravity Duality 2 Prof Nick Evans AdS/CFT Correspondence TODAY Quarks Deforming AdS Confinement Chiral Symmetry Breaking LATER Other brane games.
QCD – from the vacuum to high temperature an analytical approach an analytical approach.
Large N c QCD Towards a Holographic Dual of David Mateos Perimeter Institute ECT, Trento, July 2004.
String / gauge theory duality and ferromagnetic spin chains Rob Myers, David Mateos, David Winters Arkady Tseytlin, Anton Ryzhov M. Kruczenski Princeton.
Bottom-up AdS/QCD through a few examples Y. Kim (KIAS)
Introduction to Ads/CFT for Nuclear physicists Sang-Jin Sin (Hanyang Resort
\ String theory for Nuclear physics Sang-Jin Sin (Hanyang meeting
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.
Photo-emission in hQCD and LHC Sang-Jin Sin (Hanyang 2010/08/11.
18 May, 2003QuarkNet1 How did we come to the ideas of  quarks,  strings? Myron Bander U.C. Irvine.
Isospin effect in asymmetric nuclear matter (with QHD II model) Kie sang JEONG.
Holographic Description of Quantum Black Hole on a Computer Yoshifumi Hyakutake (Ibaraki Univ.) Collaboration with M. Hanada ( YITP, Kyoto ), G. Ishiki.
On Nuclear Modification of Bound Nucleons On Nuclear Modification of Bound Nucleons G. Musulmanbekov JINR, Dubna, Russia Contents.
1 Dynamical Holographic QCD Model Mei HUANG Institute of High Energy Physics, CAS Theoretical Physics Center for Science Facilities, CAS Seminar at USTC,
QUARK MATTER SYMMETRY ENERGY AND QUARK STARS Peng-cheng Chu ( 初鹏程 ) (INPAC and Department of Physics, Shanghai Jiao Tong University.
Photo-emission from sQGP Sang-Jin Sin (Hanyang Beijing, 2010/10/22 Based on K.Jo + SJS arXiv: X.Ge, M. Matsuo, F.Shu,T.Tsukioka,
Parton Model & Parton Dynamics Huan Z Huang Department of Physics and Astronomy University of California, Los Angeles Department of Engineering Physics.
QGP and Hadrons in Dense medium: a holographic 2nd ATHIC based on works with X. Ge, Y. Matsuo, F. Shu, T. Tsukioka(APCTP), archiv:
Nuclear Symmetry Energy in QCD degree of freedom Phys. Rev. C87 (2013) arXiv: Some preliminary results 2015 HaPhy-HIM Joint meeting Kie.
Holographic model for hadrons in deformed AdS 5 background K. Ghoroku (Fukuoka Tech.) N. Maru (U. Rome) M. Yahiro (Kyushu U.) M. Tachibana (Saga U.) Phys.Lett.B633(2006)606.
Multi-quark potential from AdS/QCD based on arXiv: Wen-Yu Wen Lattice QCD.
Sang-Jin Sin (Hanyang Univ.) Based on Archive:
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,
Plasmino and Thermal mass in hQCD: Sang-Jin Sin (Hanyang Univ. ) ATHIC 2012, Pusan Based on arXiv: To appear. Y.seo+Y.Zhou+SS For Detail,
Domain-wall/QFT correspondence Wen-Yu Wen Academia Sinica Feb 24, 2006 A Bridge Connecting Gravity and Gauge Theory.
5d truncation ignoring the 5-sphere (SO(6) gauge symmetry) There are 42 scalars - a 20 of SO(6) - a 10 and 10 of SO(6) - scalar dilaton-axion, singlets.
II Russian-Spanish Congress “Particle and Nuclear Physics at all scales and Cosmology”, Saint Petersburg, Oct. 4, 2013 RECENT ADVANCES IN THE BOTTOM-UP.
The fast life of holographic mesons Aninda Sinha Perimeter Institute, Canada. with Robert Myers arXiv:0802.nnnn Quark Matter 2008, Jaipur, India.
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.
Anthropology Series In the Beginning How did the Universe begin? Don’t know!
Heavy-quark potential at subleading order from AdS/CFT Defu Hou Huazhong Normal University, Wuhan Hou, Ren, JHEP0801:029 ( 2008 ) Chu, Hou,Ren, JHEP0908:004.
Time Dependent Quark Masses and Big Bang Nucleosynthesis Myung-Ki Cheoun, G. Mathews, T. Kajino, M. Kusagabe Soongsil University, Korea Asian Pacific Few.
Holographic QCD in the medium
Baryon Chemical Potential in AdS/CFT Shin Nakamura 中村 真 Hanyang Univ. and CQUeST (韓国・漢陽大学 ) Ref. S.N.-Seo-Sin-Yogendran, hep-th/ ( Kobayashi-Mateos-Matsuura-Myers,
And Mesons in Strange Hadronic Medium at Finite Temperature and Density Rahul Chhabra (Ph.D student) Department Of Physics NIT Jalandhar India In cooperation.
Holographic Hadrons in dense medium Sang-Jin Sin
Predictions by string theory? f 0 (1500) → 4π 0 : Suppressed Charge radius of Roper = 0.73[fm] [w/ C.I.Tan and S.Terashima, ] [w/ T.Sakai and.
Holographic cold nuclear matter as dilute instanton gas 1.Introduction 2.Model of Baryon system 3.D8 brane embedding 4.Chemical potential and phase transition.
Dynamical Instability of Holographic QCD at Finite Density Shoichi Kawamoto 23 April 2010 at National Taiwan University Based on arXiv: in collaboration.
Proton Mass and EoS for Compressed Baryonic Matter ATHIC 14/11/12 Mannque Rho (Saclay and Hanyang)
Holographic Description of Quantum Black Hole on a Computer Yoshifumi Hyakutake (Ibaraki Univ.) Collaboration with M. Hanada ( YITP, Kyoto ), G. Ishiki.
1 NJL model at finite temperature and chemical potential in dimensional regularization T. Fujihara, T. Inagaki, D. Kimura : Hiroshima Univ.. Alexander.
Andrej Ficnar Columbia University Hard Probes 2010, Eilat, Israel October 12, 2010 Nonconformal Holography of Heavy Quark Quenching Andrej Ficnar, Jorge.
Density effect and beyond
Cyrille Marquet Columbia University
Weak Interacting Holographic QCD
Physics Opportunities with heavy quark system at FAIR
Quark Mass in Holographic QCD
Some Issues in AdS/QCD Based on collaboration with
Koji Hashimoto (RIKEN, Mathematical physics lab)
Double Heavy Hadronic Spectrum from Supersymmetric LFHQCD
Finite temperature in modified Soft-Wall AdS/QCD Model
Holographic Heavy- Light mesons from non- Abelian DBI
Present status of bottom up model: sample works
Hyun Kyu Lee Hanyang University
Quark number susceptibility with finite chemical potential in hQCD
Status of AdS/QCD SangJin Sin
Excited QCD 2010, 31 Jan.-6 Feb., 2010 Tatra National Park (Slovakia)
Presentation transcript:

Nuclear Symmetry Energy in holographic QCD Sang-Jin Sin (Hanyang Univ. ) 2011.4.21@YITP Based on arXiv:1011.0868 Y.Kim, Y.Seo, I. Shin

Def: Symmetry Energy Liquid Drop Model’s Empirical formula: N=#(n), Z=#(p) It is the loss in when we go off N=Z. no linear term? Due to Isospin Invariance Turn off e&m

Physics of Es 1. Es(N-Z)^2 term is the consequence of Pauli principle. See the figure. 2.For Esinfinity: N=P For Es0, pure neutron star is possible.

Importance of Es Structure of Neutron Star The slope of the nuclear symmetry energy at saturation density is a crucial quantity to determine the mass and width of neutron-star crusts. Nucleo-Systhesis during the supernova explosion.

What is known for ? Little is known. not Exp. nor theoretical.

Why difficult? Strongly interacting. No good calculational tool in this regime. Density effect: Even lattice qcd does not help much. It is problem of tool. not imagination.

String theory idea: Replace Nuclear force by classical gravity Called ads/cft by Maldacena, Witten, GKP

z direction is warped!  ads Character of AdS/CFT I Holographic: 5d gravity theory for 4d QCD origin of +1 dim? Scale z direction is warped!  ads Stolen from Hong Liu

Character of AdS/CFT II Within the validity, Do not need loop calculation. 1. ls<<Rads 2. gs<<1 Inherit Large N theory’s Good and Bad

Character of AdS/CFT III Super-symmetry Original version is N=4 SUSY. SUSY can be broken by BC. T. d. etc Higher dim. Trade vibrational mode with KK mode. Is it QCD? Hopefully some properties will be universal. Some results are too good to be irrelevant …… [eta/s, glueon mass, ads/qcd, SS]

Gluon dynamics Geometry Gluon dynamics Geometry. Confinement or deconfinement depends on geometry.

Goemetry with BH deconfinement

Geometry with repulsive gravity Zm

Bottom up model linear sigma model in ads5. with gauged chiral symmetry SU(Nf)xSU(Nf) No potential.// BC. Instead 15% error with 3 parameter fit.

Top down model Quark: Bifundamental, D6 Meson: adjoint Dynamics: Dirac-Born-Infeld action Baryon: compact D5 D4

Model: D4/D6 +cD4 Nc D4 provide Gluonic gravity background with confinement. One compactification x4. D4 baryon vertex. 2 flavor probe brane.

Repulsive gravity for confinement set At=0 at rho=0. Then mu and Q will be related. (BH) mu=dH/dQ for DBI action. 2010/12/10

End points chargebaryon # Single Baryon Compact D-brane that wraps the transverse dimension. For D3, compact D5. for D4, compact D4 etc. Ted pole Anomally cancellation requests that Nc - F1 is attached to the probe brane D7 End points chargebaryon # D5 D3

Dense matter with baryon vertex 2010/12/10

Chemical potential set At=0 at rho=0. Then mu and Q will be related. (BH) mu=dH/dQ for DBI action. 2010/12/10

Confining metric

Dynamics of probe barne DBI action: S= Densitycharge of F, fixed chargeLegendre transformation.

DBI to Hamiltonian Hamiltonian of baryon vertex D4

Force balance between D4 D6

Main idea: asymmetry in Z-N  that in Q1-Q2

Numerical Result stiffness

Understanding For the flat embedding we can evaluate.

Stiffness For the balance, each D6 should balance the half the force. Coulomb energy

Pauli principle in hQCD. two puzzles in 4d: Driving force of Z=N is Pauli principle. Ads/cft is counting QM by classical dynamics. So how to count Pauli force. In 5d: coulomb force by charge. But charge is dual to baryon number, which is global charge. So what is dual of the coulomb force?

quark matter vs nuclear matter? From the point of view coulomb repulsion, we do not see much difference. Gluon dynamics: BH vs core bubble. Can we count the long range force of coulombic force? NOT YET!

Conclusion Symmetry Energy can be calculated using the holographic principle. Our method is the only one that can count the baryon density.

Ads/cft Dictionary Let O(x) is an color singlet operator with dimension and spin p A(x) is an source of it. Then AdS/CFT says: Extend it to d+1(=5) dim by If we know action and BC, it can be calculated CLASSICALLY. So is all correlation functions and its corollaries.

Chiral condensation and mass Mass op. is dual to a scalar Extend it to 5 dim by

Density and chemical potential In 4d, Source of baryon number op is Extend it to 5dim by

Gluon condensation and dilaton Tr(F^2) is dual to scalar Extend it to 5dim by

finally, How to detect Es ? Asymmetry in N-P is ~ that in π- π+ π-/π+ yields are sensitive to the stiffness of the symmetry energy near threshold energy. 36

Experiment 40Ca+40Ca, 96Ru+ 96Ru, 96Zr+96Zr and 197Au+197Au, and also plotted the ratios of N/Z and (N/Z)2 as a function of N/Z at incident energy 0.4A GeV and 1.5A GeV, respectively.

Meson in terms of quarks (ds) K + (us) π – (du) π 0 (uu, dd or ss) π + (ud) K – (su) K 0 (sd)