Meson Propagation in Nuclear Matter Jochen Wambach ECT*, Trento, - - PowerPoint PPT Presentation

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Meson Propagation in Nuclear Matter Jochen Wambach ECT*, Trento, - - PowerPoint PPT Presentation

Meson Propagation in Nuclear Matter Jochen Wambach ECT*, Trento, Italy Frontiers in Nuclear and Hadronic Physics Florence, February 20 to March 3, 2017 Outline I) Strong-Interaction Matter Thermodynamics Phase Transitions


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Meson Propagation in Nuclear Matter

Jochen Wambach ECT*, Trento, Italy

Frontiers in Nuclear and Hadronic Physics Florence, February 20 to March 3, 2017

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Outline

I) Strong-Interaction Matter ◮ Thermodynamics ◮ Phase Transitions ◮ Quantum-Chromodynamics ◮ The QCD Phase Diagram ◮ The Functional Renormalization Group II) Hadrons in QCD Matter ◮ The Role of Photons ◮ Dileptons in Heavy-Ion Collisions ◮ Spectral Functions from the FRG

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States of Matter

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Phase Diagram of H2O

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Landau Functions

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Matter under Extreme Conditions

early universe (∼ 10 ms) neutron star interior

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Running of the Strong Coupling Constant αs

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Mass-splitting of Parity Partners

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Symmetries of QCD and Breaking Pattern

symmetry vacuum high T low T, high µ

  • rder parameter

consequences (local) color SU(3) unbroken unbroken broken diquark condensate color super- conductivity Z(3) center symmetry unbroken broken broken Polyakov loop confinement/ deconfinement scale invariance anomaly gluon condensate scale (ΛQCD), running coupling chiral symmetry UL(Nf) × UR(Nf) = UV (1) × SUV (Nf) × SUA(Nf) × UA(1) UV (1) unbroken unbroken unbroken — baryon number conservation flavor SUV (Nf) unbroken unbroken unbroken — multiplets chiral SUA(Nf) broken unbroken broken quark condensate Goldstone bosons, no degenerate states with opposite parity UA(1) anomaly topological susceptibility violation of intrinsic parity

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Landau Functions

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’Columbia’ Plot

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Phase Diagram of QCD Matter

10-1 100 101 102 103 104

pressure

liquid gas

hadrons

mesons baryons

temperature

quarks and gluons

crossover

2SC?

C F L

chiral crystal? C E P ?

chiral phase transition 20

c

  • l
  • r
  • s

u p e r c

  • n

d u c t i n g p h a s e s

7 10 30 40 50 70 200 300 500 RHIC LHC SPS FAIR n

  • p

s u p e r f l u i d L O F F

  • p

h a s e s ?

unphysical region

1032 1033 1034 1035 1036

MeV fm

3

_

Pa MeV

K

1011 100 1012

chemical freeze out

l a t t i c e Q C D

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Phase Diagram of QCD Matter

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Flow

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Flow

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Momentum Flow of the Effective Potential

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Phase diagram of the Quark-Meson Model

◮ chiral order parameter σ0 decreases towards higher T and µ ◮ a crossover is observed at T ≈ 175 MeV and µ = 0 ◮ critical endpoint (CEP) at µ ≈ 292 MeV and T ≈ 10 MeV ◮ vacuum: σ0 = 93.5 MeV, mπ = 138 MeV, mσ = 509 MeV, mq = 299 MeV

100 200 300 400 Μ MeV 50 100 150 200 250 T MeV

270 290 310 5 10 15 20

[R.-A. T., N. Strodthoff, L. v. Smekal, and J. Wambach, Phys. Rev. D 89, 034010 (2014)] 17 / 42

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Generation of Mass in QCD

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Temperature Evolution of the Chiral Condensate

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Mass-splitting of Parity Partners

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Heavy-ion Collisions and Photons

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e+e− - annihilation in the vaccum

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Vector-meson Selfenergies

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Spectral Function

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Photo-absorption as a Test

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In-medium ρ-meson under HIC conditions

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Spectral Function weighted by 1/M

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Dilepton Rates

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Dilepton Rates and the Phase Diagram

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Dilepton Data CERES

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Dilepton Data STAR

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Dilepton Data SPS NA60

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Dilepton Data SPS NA60

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Flow Equations for Mesonic Two-point Functions

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Flow of the Sigma and Pion Spectral Functions in vaccum at q = 0

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Sigma and Pion Spectral Function with increasing T at µ = 0 and q = 0

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Sigma Spectral Function with increasing T at µ = 0

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Pion Spectral Function with increasing T at µ = 0

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Flow Equations for Vector-Meson Two-point Functions

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ρ and a1 Spectral Function with increasing T at µ = 0 and q = 0

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ρ and a1 Mass Flow

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ρ and a1 Pole Masses

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