Chiral Symmetry Restoration and Deconfinement in Neutron Stars - - PowerPoint PPT Presentation

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Chiral Symmetry Restoration and Deconfinement in Neutron Stars - - PowerPoint PPT Presentation

Chiral Symmetry Restoration and Deconfinement in Neutron Stars Vernica Dexheimer 1. Motivation Having a model that can be used for: small temperatures and high densities neutron stars high temperatures and small densities heavy ion


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Chiral Symmetry Restoration and Deconfinement in Neutron Stars

Verônica Dexheimer

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  • 1. Motivation

Having a model that can be used for:

– small temperatures and high densities – high temperatures and small densities – everything in the middle

Include different degrees of freedom in the

same model Study chiral symmetry restoration and deconfinement to quark matter inside compact stars

neutron stars heavy ion collisions

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  • 2. Chiral Model

<>  

_

M

scalar term breaks symmetry M L R R L M

Effective mass comes from coupling to field

  M*

 M*=g 

QCD vacuum filled with qq pairs (not chiral invariant!)

_

_

_

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The chiral symmetry is restored earlier (smaller chemical potential) for higher temperatures.

Chiral Condensate  (B,T)

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  • Appearance of heavier (strange) particles as

density increases hyperons

  • Amount of each particle not constant
  • Chemical equilibrium

p, n, , +, 0, -, 0, - ++, +, 0, - , *+, *0, *-, *0, *-,  n  p + e + e

_

e, 

  • Leptons ensure charge neutrality
  • 3. Composition
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e, 

  • Deconfinement of hadrons
  • New degrees of freedom: quarks
  • Chiral symmetry restoration

increase of density B

u, d, s

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  • 4. Non Linear Sigma Model (hadrons)

=0

frozen limit:

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Same model for hadrons and quarks Introduce a potential for  at any density and temperature

no quarks no hadrons

  • 5. Inclusion of Quarks in the Model

mesons

  • rder parameter for deconfinement

in analogy with the Polyakov loop

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The first order phase transition line ends at a critical point.

μc=354 MeV Tc=167 MeV μc=1345 MeV ρB=4 ρ0

  • 6. Phase Diagram

HADRONIC PHASE BROKEN CHIRAL SYMMETRY QUARK PHASE RESTORED CHIRAL SYMMETRY

B

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First order phase transition for  and the chiral condensate.

  • 7. Hybrid Stars (T=0)
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No mixed phase: just hadron matter or quark matter.

Population (local charge neutrality)

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With the inclusion of a quark phase the maximum mass of the star decreases from 2.1 to 1.9M⊙.

Mass-Radius Diagram

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Presence of mixed phase.

Population (global charge neutrality)

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  • 8. Magnetic Field
  • In the z direction and dependent on the

chemical potential

  • Quantization of the energy levels in the x and y

directions for the charged fermions until

69.25 MeV2=1015G

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B increases toward the center of the star.

1MeV 2 = 1.444 x 1013 G

Effective Magnetic Field

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EOS becomes softer and eventually unphysical with the increase of B.

Equation of State

1MeV 2 = 1.444 x 1013 G

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Stars become less massive with the increase of B.

1MeV 2 = 1.444 x 1013 G

Mass-Radius Diagram

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We can evaluate how chiral symmetry is restored and how deconfinement occurs since the degrees of freedom change naturally in our model from hadrons ↔ quarks We reproduce the physics of the entire phase diagram including lattice QCD, heavy ion collisions, nuclear physics and neutron star results For zero temperature (with global charge neutrality) we reproduce a mixed phase that allows stable (massive) star configurations with presence of hybrid matter up to 2 km The pressure behaviour establishes a limit for the magnetic field The presence of strong magnetic field allows deconfinement to happen at smaller chemical potential but reduces the mass

  • f the respective star
  • 9. Conclusions
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Apply the model to supernova matter to analyse how neutrino trapping affects the results Analyse the effect of magnetic field in the phase diagram:

– proto-neutron stars – heavy ion collisions

Outlook