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Hadron to Quark Phase Transition in the Global Color Symmetry Model of QCD

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 D.F., Chang L. Wang B., Song H.C., Chao J.Y. et al., at PKU;

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Hadron to Quark Phase Transition in the Global Color Symmetry Model of QCD

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  1. 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 D.F., Chang L. Wang B., Song H.C., Chao J.Y. et al., at PKU; Wang F., Zong H.S., et al., at NJU; Lue X.F. at SCU; Zhao E.G. at ITP; Chao W.Q. at IHEP.

  2. Outline I. Introduction II. The Framework III. Numerical Results IV. Remarks

  3. I. Introduction Two Puzzles in Current Physics (in T.D. Lee’s words):  Chiral Symmetry and its Spontaneous Breaking Color Confinement • Characteristics Identifying Quark Deconfinement and Chiral Symmetry Restoration: Hadron Properties Vacuum Structure Lattice QCD, pQCD (Factorization, Re-summation), ••• Confinement Mechanism: Flux Tube, Center Vertex, ··· Intuitive view? NJL model, QMC, QMF, Truncated DSE, Instanton, GCM, ···

  4. How the Chiral Symmetry is Restored ? Quark condensates are usually taken as characteristics of Vacuum Structure Order Parameters. Theoretical approaches: Composite-operator, Sum rules, QMC, Walecka model, Dirac-Brueckner, S-D Equation, Instanton dilute liquid model, … Different results have been obtained!! Chi. Sym. C S B

  5. (Comp.-Op., PRD41,1610(’90) ) ( QSR, NP A642, 171 (’98) ) (Walecka, PR C55, 521 (‘97)) (D-S Eq. PR C55, 1577(’97) ) (IDLM, NP A642, 83(’98) ) (DS Eq. PR C57, 2821(’98) )

  6. Hadron Properties are essential in describing finite nuclei and strong interaction matter  Effective mass EMC effect, nuclear structure & reaction  Nucleon swell EMC effect  Bag constant Quark confinement Theoretical Approaches: Bag Models, QMC, QMF bag constant, bag energy, radius Phenomenologically! QCD foundation ??? the GCM appears

  7. II. The Framework of the GCM 1. The Main Point of Global Color Symmetry Model R.T. Cahill, C.D. Roberts, Phys. Rev. D 32 (1985) 2419

  8. Lue, Liu, Zhao, Zong, Phys. Rev. C 58 (1998) 1195 Effective degrees of freedom becomes quark and chiral mesons Prog. Part. Nucl. Phys. 39 (1997) 117; Phys. Rev. D49 (1994) 125; Phys. Rev. C53 (1996) 2410; ······ .

  9. 2. GCM in Strongly Interacting Matter

  10. 3. The Scalar Quark Condensates

  11. 4. The mass and decay constant of pion

  12. 5. Relation Between the Chemical Potential and the Density

  13. GCM, Global Color Symmetry Model: an effective field theory model of QCD Truncated DSE NJL, ChPT QCD GCM Hadronisation Observables BM, QMC, QHD Lattice Hadron Correlation With the GCM, one can explore the QCD foundation of bag models, the chiral symmetry breaking and restoration, the quark confinement and deconfinment, ••••••••••.

  14. III. Numerical Results New approach to determine the vacuum configuration of the GCM B = m in instanton model Property of pion and sigma meson Lue, Liu, Zhao, Zong, Phys. Rev. C 58 (1998) 1195

  15. Relation between  and 

  16. Nucleon bag constant Y. X. Liu, et al, Nucl. Phys. A 695 (2001) 353, A 725 (2003) 127 B(0)=(172 MeV)4

  17. Nucleon radius and mass R(0)=0.7 fm m(0)=939 MeV Y. X. Liu, et al, Nucl. Phys. A 695 (2001) 353; A725 (2003) 127.

  18. Quark condensatesIn nuclear matter Y. X. Liu, et al, Phys. Rev. C68 (2003), 035204.

  19.  With a full gluon propagator - relationnucleon properties Y. X. Liu, et al, Nucl. Phys. A 750 (2005), 324.

  20. quark condensate

  21. Quark Gluon mixed Condensate Zhao Zhang, Wei-qin Chao, Phys. Lett. B 610 (2005), 235

  22. The effective potential at and quark confinement results from the self-adjustment among/between quarks

  23. The effective potential at finite and quark deconfinement and chiral symmetry restoration may take place

  24. The mass and decay constant of pion

  25. Susceptibilities: Zong H. S. et al., Phys. Lett. B 557 (2003) 33 Zong H. S. et al., Phys. Lett. B 576 (2003) 289 Zong H. S. et al., Phys. Rev. D 67 (2003) 074004 Zhang Z., Chao W.Q., Phys. Lett. B 612 (2005) 207 Axial vector vertex Zong H. S. et al., Phys. Rev. C 66 (2002) 015201 New Approach to Evaluate the Quark Propagator at Finite Chemical Potential Zong, Chang, Hou, Sun, Liu, Phys. Rev. C 71 (2005) 015205

  26. IV. Remarks  The density dependence of the bag constant, the mass and radius of nucleons and the pion mass and decay constant are studied in an effective field theory model of QCD,namely the GCM  The scalar local and nonlocal quark condensates are also investigated.  Calculated result 1: with the increase of the density before a critical value is reached, the BN and MN decrease, the M almost maintains constant, the RN, the f and the condensates increase.

  27.  Calculated result 1: with the increase of the density • before a critical value is reached, the BN and MN decrease, • the M almost maintains constant, the RN, , , • the f and the condensates increase.  Calculated result 2: at the critical density, the BN and MN vanish gradually, the M , f and the , etc, disappear suddenly, the RN becomes infinite.  Quark deconfinement and the chiral symmetry restoration phase transitions happen at the critical density.  Chiral symmetry restoration process: broken more strongly gradually, at least, at the same scale, then restored suddenly.

  28. Thanks !!!

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