the structure of neutron star by using the quark-meson coupling model
DESCRIPTION
The structure of neutron star by using the quark-meson coupling model. Heavy Ion Meeting (2008. 11. 14) C . Y. Ryu Soongsil University, Korea. Outline. 1. Introduction and motivation - Structure of neutron star - Mass and radius relation - The observed masses of neutrons star - PowerPoint PPT PresentationTRANSCRIPT
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The structure of neutron star by using the quark-me-
son coupling model
Heavy Ion Meeting (2008. 11. 14)C. Y. Ryu
Soongsil University, Korea
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Outline1. Introduction and motivation
- Structure of neutron star- Mass and radius relation- The observed masses of neutrons star- Motivation
2. Theory- Quark-meson coupling model (dense mat-ter)- Exotic phases
: hyperons, kaon condensation- Finite temperature
3. Results
4. Summary
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1.Introductionand
motivation
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Hot and dense matter I- Heavy ion collision
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Hot and dense matter II- Proto-neutron star
The structure of supernovae The production of proto-neutron star
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The production of neutron star
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The structure of neutron star
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A. Van der Meer et al., astro-
ph:0707.280201(2007)1) Best fit : 1.35 M⊙
2) Recent observations : large masses
The observed massesMaybe, black-hole
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Motivation I
1) No strangeness : 2-3 M๏
2) Strangeness : 1-2 M๏ - hyperons(Λ, Σ, Ξ) - kaon condensation - quark matter(u, d, s)
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KEK PS-E471 (2004)
Deep optical potential V0 ≈ -120 MeV
Y. Akaishi & T. Yamazaki, PRC65 (2002)N. Kaiser, P.B. Siegel & W. Weise, NPA594 (1995)
J. Mares, E.Friedman and A. Gal,Nucl.Phys.A770 (2006)
Ramos & E. Oset, Nucl. Phys. A671 (2000)V. K. Magas, E.Oset, A.Ramos, H.Toki, nucl-th/0611098
Chirally-motivated potentials
Shallow optical potential V0 ≈ -50 MeV
Motivation II - Deeply bound kaonic nuclear states
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• Model dependency - Haron degree of freedom : Quantum Hadrodynamics (QHD)
- Quark degree of freedom : Quark-meson coupling model (QMC) model
σ, ω
σ, ω
Motivation III
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2. Theory
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Quark-meson coupling model
- MIT bag + mean fieldsQuark-meson cou-
pling (QMC) model
MIT bag + σ, ω mesons
σ, ωNeutron star
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Saturation density 0 = 0.17 fm-3
Binding energy B/A = ε/ρ – m N = 16 MeV Effective mass of a nucleon m N*/m N = 0.7 - 0.8
(0.78) Compression modulus K-1 = 200 - 300 MeV Symmetric energy asym= 32.5 MeV
The QMC model at saturation1) Infinite, static and uniform matter
2) The properties of nuclear matter
3) The Lagrangian of QMC model for infinite nuclear mat-ter
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QMC model for hyperonic matter
σ–ω–ρ(only u(d) quark) + σ*(980) –φ(1050) (only s quark)
Lagrangian density for baryon octet and leptons
Baryon octet : p, n, Λ, Σ+, Σ0, Σ-, Ξ0, Ξ-, lepton : e, μ
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Naive picture of K- potential
udd
uu
1) OZI rule : s-quark does not interact with u and d quarks
p p2) Antiparticle may feel very strong attraction.
3) Potential of particle Scalar (attractive)+ Vector (repulsive)
4) Potential of antiparticle – strong attraction Scalar (attractive)+ Vector (attractive)
σ, ω
K-
uSu
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Strong force of K- N and kaon condensation
K- pp system
Kaon condensation in medium
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The RMF for kaon and antikaonLagrangian density for baryon octet and leptons
Langrangian density for kaon
The potential of K- : UK- = - gσ – g ω0
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The QMC model at finite temperature1. Thermodynamic grand potential :
Ω = ε – TS - μρ2. Pressure is
Where
3. The condition for equilibrium – minimize Ω or maximize P.
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TOV equation• Macroscopic part – General relativity
• Microsopic part – QMC model
• Einstein field equa-tion :
Static and spherical symmetric neutron star (Schwarzschild metric)
Static perfect fluidDiag Tμν = (ε, p, p, p)
• TOV equation :
• equation of state (pressure, energy density)
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The conditions in neutron star
1) Baryon number conservation :
2) Charge neutrality :
3) chemical equilibrium (Λ, Σ, Ξ)
μK = μe
※ The condition for K- condensa-tion
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Eq. of state in kaon+hyperonic mat-ter
The energy density :
The pressure :
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3. Results
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The population of particles in neutron star
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The population of particles in neutron star
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The population of particles in neutron star
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The mass of a neutron star andkaon condensation
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σmeson fields at finite tem-perature
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The effective masses of a nucleon at finite tempera-
ture
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Summaries1. Hadronic phases : QHD and QMC models
i) Proto-neutron star – 2.0 solar massii) Hyperons - 1.6-7 Solar massiii) Kaon condensation – 1.4-5 solar mass
But, we can see the model dependency in both.
2. All results depend on the coupling constants and the potentials of kaon and baryons.
– Experiment has to confirm them.
3. If the observed mass is larger than 2.0 solar mass, all exotic phases are ruled out(?).
4. Finite temperature – symmetric matter