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Structure of Spin Polarized S trange Q uark S tar in the Presence of Magnetic Field at Finite Temperature @arXiv 1301:0899. Reporter: Long Jiang Nanjing University. Outline. Introduction Why SQS Properties of SQS Background of this paper Equation of State Spin polarized
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Structure of Spin Polarized Strange Quark Star in the Presenceof Magnetic Field at Finite Temperature @arXiv 1301:0899 Reporter: Long Jiang Nanjing University
Outline • Introduction Why SQS Properties of SQS Background of this paper • Equation of State Spin polarized In presence of strong magnetic field At finite temperature • Some results and discussion
Introduction — Why SQS? • Landau’s neutron star • Witten: SQM stable than nuclei • Density: ~10^15 g/cm^3 • Mass: 2.1+-0.28Ms • Magnetar ( SGRs & AXPs) • CCO • XDIN
Other Properties of SQS • Density of core & base of the crust • Ultra-high electric field: ~15% of mass • Ultra-high magnetic field: ~5% of mass • Rapid rotation • · · · Candidates: SAX J1808.4-3658, EXO 1785-248, 3C58 4U 1608-52, 4U 1820-30, RX J185635-3754
Background of this paper • Influence of magnetic field Equation of State Maximum mass Gravitational red-shift • Used model: MIT bag model Density dependent bag constant: B
Structure description Equation of State: p=?
Equilibrium SQM: up, down, strange quarks & e
To get the EoS (1) Polarization Number density Energy
Other results Max: Min: Near the red-shift of RX J185635-3754: zs ~ 0.35