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Quark star RX J1856.5-3754 and its mass
Kazunori Kohri (郡 和範) RESCEU, Univ. of Tokyo K. Kohri, K. Iida and Katsuhiko Sato, Prog. Thor. Phys. 105 (2002) in press
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Contents ・ Introduction ・ Observations of RX J1856.5-3754
・ Two-temperature model? ・ Quark matter in bag model ・ Quark star ・ Systematic study of mass of the star in bag model ・ Other constraint on mass of the star ・ Other theoretical model of quark matter ・ Conclusion
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Introduction Recent deep Chandra LETG+HRC-S observations of RX J reports, Drake et al., ApJ. 572 (2002) Black body of X-ray luminosity, Radiation radius
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Distance toward RX J Drake et al., ApJ. 572 (2002)
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Spectra of RX J Drake et al., ApJ. 572 (2002)
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The 3σequivalent width upper limit to line features
Drake et al., ApJ. 572 (2002)
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XMM-Newton observation
V. Burwitz et al, astro-ph/
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RX J1856.5-3754 is quark star? i) No pulsation
ii) No spectral features iii) Small radiation radius
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Mass-radius relation of compact star
(Quark star) (White dwarf) (Neutron star) M R Courtesy of K. Iida
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Two temperature model Cold with heavy-element atmosphere
F.Walter and J.Lattimer, ApJ (2002) T.M. Braje and R.W. Romani, ApJ (2002) X-ray Hot Cold UV/Optical Hot X-ray
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Broad band spectral fit in two-temperature blackbody
T. Braje and R.W. Romani, ApJ (2002)
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Quark matter (zero-temperature uds quark matter)
Thermodynamic potential Energy density QCD coupling constant where Strange quark mass Bag constant
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Quark matter-2 Number density Pressure Baryon number Conditions
In equilibrium through weak interactions Charge neutrality
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Bag model parameters fitted to hadron mass spectra
Kohri, Iida and Sato, arXiv:astro-ph/
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Energy per baryon (αc=0)
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Energy per baryon (αc=0.6)
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Equation of state
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Quark star Equation of hydrostatic equilibrium
(Tolman-Oppenheimer-Volkoff (TOV) equation) Equation of mass conservation Then, the radius is determined by The mass is
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Mass of quark star
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Radius of quark star
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Mass-radius relation
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Mass-radius relation
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Observed X-ray luminosity
Bondi accretion rate where, Then,
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Contours of upper limit of mass
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Effects of the pressure-dependent bag constant
Generally, we can parameterize the EOS as A ~ , for Lattice data , Peshier,Kampfer,Soff (2001). A ~ 2, for Relativistic Mean Field, Dey et al. (1998) etc. Then, we transform it into where Namely, inside the star the bag constant effectively becomes large!
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Contour of the effective bag constant
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Contours of the upper limint of the mass
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Conclusion ・We have systematically computed mass-radius relation of quark star within the bag model. ・ Assuming that RX J is a pure quark star, we have derived an upper limit on its mass. ・ We find the upper limit can amount to 1 M around B ~ (200MeV). 4
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