Chiral Symmetry Restoration and Deconfinement in QCD at Finite Temperature M. Loewe

1. Chiral Symmetry Restoration and Deconfinement in QCD at Finite Temperature M. Loewe Pontificia Universidad Católica de Chile XVIII Simposio Chileno de Física. La Serena, Noviembre 2012

2. This talk is based on the following article: Chiral symmetry restoration and deconfinement in QCD at finite temperature: C. A. Dominguez, M. Loewe and Y. Zhang. Hep-ph 1205.336. Phys. Rev. D. 86 (2012) 034030 I acknowledge support form : FONDECYT 1095217 and Proyecto Anillos ACT119 (CHILE)

3. There are two (at least two) phase transitions that may occur in QCD at finite temperature and/or density: • Deconfinement due to color screening • Chiral symmetry restoration: Moving from a Nambu-Goldstone to a Wigner-Weyl realization Which are the relevant order parameters in each case? Both transitions seem to occur approximately at the same temperature

4. An order parameter is a quantity that vanishes in a certain phase, being finite in a second one. The relevant physical variables are temperature (T) and baryon chemical potential (μB) General Aspects: Normally the Polyakov loop (confinement) and the quark condensate (chiral symmetry restoration) are used as order parameters When μB = 0 and T ≠ 0 lattice results provide a consistente picture, resulting in a similar Tc for both transitions in the range 170 MeV < Tc < 200 MeV (finite quark masses) However…..

5. For finite Baryon Chemical Potential, the fermion determinant becomes complex and lattice simulations are not possible. So, perhaps we need a new variable, instead of the Polyakov Loop, for discussing deconfinement. An attractive possibility: the continuum threshold of the hadronic resonance spectral function. Phenomenological order parameter. This discussion can be done in the frame of the extended (finite T and μB) QCD Sum Rules program

6. Realistic Spectral Function Im Π s0 s ≡ E2

7. Realistic Spectral Function (T) Im Π S0(T) s ≡ E2

8. For this purpose we will use QCD Sum Rules. OPERATOR PRODUCT EXPANSION OF CURRENT CORRELATORS AT SHORT DISTANCES (BEYOND PERTURBATION THEORY) CAUCHY’S THEOREM IN THE COMPLEX ENERGY (SQUARED) S-PLANE

9. We reconsider the light quark axial-vector channel, using the first three FESR, together with an improved spectral function Π0(q2) and Π1(q2)are free of kinematical singularities

10. Invoking the OPE No evidence for d=2 at T=0. The dimension d=4 is given by The second term is negligible compared with the gluon condensate

11. The normalization of the correlator in PQCD In the hadronic sector we have the pion pole followed by the a1(1260) resonance A good fit to the ALEPH data is given by

12. rt Ma1 = 1.0891 GeV, Γa1 = 568.78 MeV, C fa1 = 0.048326. From the first Weinberg Sum Rule we get f a1 = 0.073 → C = 0.662

13. Thermal Extension of the QCD Sum Rules • There are important differences: • 1) The vacuum is populated (a thermal vacuum) • 2) A new analytic structure in the complex s-plane appears, due to scattering. This effect turns out to be very important

14. Finite Temperature Effects 1) Time-like region: ω2 - │q │2 > 0 2) Space-like region: ω2 - │q │2 < 0

15. uark condensate h¯qqi(T )/h¯qq f2 (T )/f2 (0) as a function of T/Tc in the chiral limit (mq = M = 0) with Tc = 197 Me Previous Information Tc = 197 MeV Evolution of the quark condensate (equivalent to fπ). The solid line (Schwinger-Dyson approach) is chiral limit. Dotted line is for massive quarks (Lattice data)

16. We will concentrate on the chiral limit, as we find that the FESR have only solutions up to 0.9 Tc where the quark condensate is essentially unique. Gluon Condensate

17. The first three sum rules: 1) 2)

18. 3) From these Sum Rules, we are able to get: S0(T); fa1(T); Γa1(T) Assumption: ma1 does not depend on T

19. fπ2(T) / fπ2(0): Dotted curve. S0(T) / S0(0): Solid curve.

20. The width definitely grows with temperature

21. The coupling decreases!!

22. Conclusions: We have confirmed the picture where S0(T) moves to the left, being a phenomenological order parameter for deconfinement deconfinement. The width of the a1 has a divergent behavior as function of T. The coupling fa1 (T) vanishes at the critical temperature.