Plasmino in graphene at finite temperature? Daqing Liu Changzhou University, China.

Slides:

Advertisements

Similar presentations

A method of finding the critical point in finite density QCD

Advertisements

Mass, Quark-number, Energy Dependence of v 2 and v 4 in Relativistic Nucleus- Nucleus Collisions Yan Lu University of Science and Technology of China Many.

Elliptic flow of thermal photons in Au+Au collisions at 200GeV QNP2009 Beijing, Sep , 2009 F.M. Liu Central China Normal University, China T. Hirano.

From weak to strong correlation: A new renormalization group approach to strongly correlated Fermi liquids Alex Hewson, Khan Edwards, Daniel Crow, Imperial.

Hard Photon Production in a Chemically Equilibrating QGP at Finite Baryon Density Zejun He Zejun He Shanghai Institute of Applied Physics Research Chinese.

Quantum Harmonic Oscillator for J/psi Suppression at RHIC and SPS Carlos Andrés Peña Castañeda Institute of Theoretical Physics, University of Wrocław,

Calculation of Dielectric Function of a Quark-gluon Plasma Jiang Bing-feng Li Jia-rong IOPP CCNU

Plasmonics in double-layer graphene

Chiral symmetry breaking in graphene: a lattice study of excitonic and antiferromagnetic phase transitions Ulybyshev Maxim, ITEP, MSU.

N F = 3 Critical Point from Canonical Ensemble χ QCD Collaboration: A. Li, A. Alexandru, KFL, and X.F. Meng Finite Density Algorithm with Canonical Approach.

Two-particle Distribution and Correlation in Hot QGP Hui Liu （刘绘） Phys. Dep., JiNan University Jiarong Li （李家荣） IOPP, CCNU Outline: Brief review on distribution.

Bound-Free Electron-Positron Pair Production Accompanied by Coulomb Dissociation M. Yılmaz Şengül Kadir Has University & İstanbul Technical University.

J. RuppertFocus talk on interactions between jets and medium #1 Focus talk on interactions between jets and medium Jörg Ruppert Nuclear Theory, Duke University.

Dilepton production in HIC at RHIC Energy Haojie Xu( 徐浩洁 ) In collaboration with H. Chen, X. Dong, Q. Wang Hadron2011, WeiHai Haojie Xu( 徐浩洁 )

Universal thermodynamics of a strongly interacting Fermi gas Hui Hu 1,2, Peter D. Drummond 2, and Xia-Ji Liu 2 1.Physics Department, Renmin University.

Chiral Magnetic Effect on the Lattice Komaba, June 13, 2012 Arata Yamamoto (RIKEN) AY, Phys. Rev. Lett. 107, (2011) AY, Phys. Rev. D 84,

M. Djordjevic 1 Effect of dynamical QCD medium on radiative heavy quark energy loss Magdalena Djordjevic The Ohio State University.

M. Djordjevic 1 Heavy quark energy loss in a dynamical QCD medium Magdalena Djordjevic The Ohio State University M. Djordjevic and U. Heinz, arXiv:

University of Catania INFN-LNS Heavy flavor Suppression : Langevin vs Boltzmann S. K. Das, F. Scardina V. Greco, S. Plumari.

QCD Phase Diagram from Finite Energy Sum Rules Alejandro Ayala Instituto de Ciencias Nucleares, UNAM (In collaboration with A. Bashir, C. Domínguez, E.

Consider a time dependent electric field E(t) acting on a metal. Take the case when the wavelength of the field is large compared to the electron mean.

Gluon Propagator and Static Potential for a heavy Quark-antiquark Pair in an Anisotropic Plasma Yun Guo Helmholtz Research School Graduate Days 19 July.

Quantum Field Theoretic Description of Electron-Positron Plasmas Markus H. Thoma Max-Planck-Institute for Extraterrestrial Physics, Univ. Giessen, MAP,

The J/  as a probe of Quark-Gluon Plasma Erice 2004 Luciano MAIANI Università di Roma “La Sapienza”. INFN. Roma.

Physics of fusion power Lecture 3: Lawson criterion / Approaches to fusion.

QM 年 11 月日 Shanghai, China 梁作堂 (Liang Zuo-tang) 山东大学 1 For The 19th International Conference on Ultra-Relativistic Nucleus-Nucleus Collisions.

Test Z’ Model in Annihilation Type Radiative B Decays Ying Li Yonsei University, Korea Yantai University, China Based on J. Hua, C.S Kim, Y. Li, arxiv:

Lecture Dirac 1927: search for a wave equation, in which the time derivative appears only in the first order ( Klein- Gordon equation:

Lattice Fermion with Chiral Chemical Potential NTFL workshop, Feb. 17, 2012 Arata Yamamoto (University of Tokyo) AY, Phys. Rev. Lett. 107, (2011)

Effect of thermal fluctuation of baryons on vector mesons and low mass dileptons ρ ω Sanyasachi Ghosh (VECC, Kolkata, India)

Study of the QCD Phase Structure through High Energy Heavy Ion Collisions Bedanga Mohanty National Institute of Science Education and Research (NISER)

P. Gubler, K. Morita, and M. Oka, Phys. Rev. Lett. 107, (2011) K. Suzuki, P. Gubler, K. Morita, and M. Oka, arxiv: [hep-th]

Luan Cheng (Institute of Particle Physics, Huazhong Normal University) I.Introduction II. Potential Model with Flow III.Flow Effects on Parton Energy Loss.

Locating critical point of QCD phase transition by finite-size scaling Chen Lizhu 1, X. S. Chen 2, Wu Yuanfang 1 1 IOPP, Huazhong Normal University, Wuhan,

Drude weight and optical conductivity of doped graphene Giovanni Vignale, University of Missouri-Columbia, DMR The frequency of long wavelength.

Hadron-Quark phase transition in high-mass neutron stars Gustavo Contrera (IFLP-CONICET & FCAGLP, La Plata, Argentina) Milva Orsaria (FCAGLP, CONICET,

Review of recent highlights in lattice calculations at finite temperature and finite density Péter Petreczky Symmetries of QCD at T>0 : chiral and deconfinement.

1 QCD Thermodynamics at High Temperature Peter Petreczky Large Scale Computing and Storage Requirements for Nuclear Physics (NP), Bethesda MD, April 29-30,

Fluctuation effect in relativistic BCS-BEC Crossover Jian Deng, Department of Modern Physics, USTC 2008, 7, QCD workshop, Hefei  Introduction  Boson-fermion.

Study of chemical potential effects on hadron mass by lattice QCD Pushkina Irina* Hadron Physics & Lattice QCD, Japan 2004 Three main points What do we.

How To See the Quark-Gluon Plasma

CPOD2011 ， Wuhan, China 1 Isospin Matter Pengfei Zhuang Tsinghua University, Beijing ● Phase Diagram at finite μ I ● BCS-BEC Crossover in pion superfluid.

PHOTONS AND EVOLUTION OF A CHEMICALLY EQUILIBRATING AND EXPANDING QGP AT FINITE BARYON DENSITY Shanghai Institute of Applied Physics Jiali Long, Zejun.

Probing QGP by Heavy Flavors Santosh Kumar Das Theoretical Physics Division.

Heavy Quark Energy Loss due to Three-body Scattering in a Quark- Gluon Plasma Wei Liu Texas A&M University  Introduction  Heavy quark scattering in QGP.

Search for QCD Critical Point at RHIC Bedanga Mohanty National Institute of Science Education and Research (NISER) Outline:  Phase diagram of QCD  Observables.

BFKL equation at finite temperature Kazuaki Ohnishi (Yonsei Univ.) In collaboration with Su Houng Lee (Yonsei Univ.) 1.Introduction 2.Color Glass Condensate.

Mean Field Effect on J/psi Production in Heavy Ion Collisions Baoyi Chen Physics Department Tsinghua University Cooperators: Kai Zhou Yunpeng Liu Pengfei.

THERMODYNAMICS OF THE HIGH TEMPERATURE QUARK-GLUON PLASMA Jean-Paul Blaizot, CNRS and ECT* Komaba - Tokyo November 25, 2005.

Quarks Quarks in the Quark-Gluon Plasma Masakiyo Kitazawa (Osaka Univ.) Tokyo Univ., Sep. 27, 2007 Lattice Study of F. Karsch and M.K., arXiv:

Helmut Satz and the Formative Days of RHIC T. Ludlam June 9, 2011.

What does HTL lose? Hui Liu Jinan University, China.

Hot 1-2 Loop QCD*** B. Kämpfer Research Center Dresden-Rossendorf Technical University Dresden ***: M. Bluhm, R. Schulze, D. Seipt real, purely imaginary.

M. Djordjevic 1 Heavy quark energy loss in a dynamical QCD medium Magdalena Djordjevic The Ohio State University M. Djordjevic and U. Heinz, arXiv:

PHENIX Results from the RHIC Beam Energy Scan Brett Fadem for the PHENIX Collaboration Winter Workshop on Nuclear Dynamics 2016.

Higgs Bosons in Condensed Matter Muir Morrison Ph 199 5/23/14.

Production, energy loss and elliptic flow of heavy quarks at RHIC and LHC Jan Uphoff with O. Fochler, Z. Xu and C. Greiner Hard Probes 2010, Eilat October.

Analysis of the anomalous tail of pion production in Au+Au collisions as measured by the PHENIX experiment at RHIC M. Nagy 1, M. Csanád 1, T. Csörgő 2.

Lattice gauge theory treatment of Dirac semimetals at strong coupling Yasufumi Araki 1,2 1 Institute for Materials Research, Tohoku Univ. 2 Frontier Research.

1 NJL model at finite temperature and chemical potential in dimensional regularization T. Fujihara, T. Inagaki, D. Kimura : Hiroshima Univ.. Alexander.

Deconfinement and chiral transition in finite temperature lattice QCD Péter Petreczky Deconfinement and chiral symmetry restoration are expected to happen.

Heavy quarks and charmonium at RHIC and LHC within a partonic transport model Jan Uphoff with O. Fochler, Z. Xu and C. Greiner XLIX International Winter.

Review of ALICE Experiments

Oleg Pavlovsky (ITPM MSU)

NGB and their parameters

The Study of the Possible Phase Diagram of Deconfinement in FL Model

Properties of the Quark-Gluon Plasma

GLOBAL POLARIZATION OF QUARKS IN NON-CENTRAL A+A COLLISIONS

QCD at very high density

A possible approach to the CEP location

Presentation transcript:

plasmino in graphene at finite temperature? Daqing Liu Changzhou University, China

Outline  Collective Excitations in hot QCD  Possible collective excitations in warm graphene  Outlook

 In QCD, about T>150Mev, there is a first phase transition (QCDPT). i.e., L.S. Kisslinger and D. Das, arXiv:

Two ways to get so high temperature  Early universe  Latent heat. heavy ion collision, RHIC and LHC

Plasmon In QGP, there are two collective excitations Plasmino

Some literatures on plasmino

arXiv: arXiv: arXiv:hep-ph/

Possilbe collective excitations in graphene

Possible collective excitations in warm graphene  Plasmon 1) F.H.L. Koppens, D.E. Chang and F.J.G. de Abajo, Graphene plasmonics: A platform for stron Light-matter interactions, Nano Lett. 11, 3370 (2011) 2) S.D. Sarma and E.H. Hwang, Collective modes of the massless Dirac plasma, Phys.Rev.Lett. 102, (2009) 3) Y. Liu, R.F. Willis, K.V. Emtsev and T. Seyller, Plasmon dispersion and damping in electrically isolated two-dimesenional charge sheets, Phs. Rev. B (R) (2008) 4) S.D. Sarma and Q. Li, Intrinsic plasmon in 2D Dirac materials, Phys. Rev. B. 87, (2013)

Propagators  Fermion  where  Potential

Feynman diagram for carrier self-energy correction We also focus on the case As for the correction from temperature, there are two cases, High temperature, Debye screening Low temperature (The influence of T on V is neglected)

Phys. Rev. B 85, (2012) Phys.Lett. B359 (1995)

This is the main challenge of the topic. We set To calculate the correction we introduce invariants We have and the domain of the integration and ，

The scalar part, which is an odd function of, The self-energy correction can be divided into two parts, The spinor part, which is an even function of, ？

In RPA, the full carrier propagator is The zero point is at

T=0.3

To simplify the discussion, we assume We have two solutions T=0.5

T=0.3. The fit curve is The difference between with 0.06 term and wothout 0.06 term

Outlook  Graphene: The TRUE bridge between high- and low-energy physics  The (anti-)plasmino states in graphene can help us to understand (anti-)plasmino in QGP and hot QCD.

Thanks for your attention