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奇异星性质的研究
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摘要
如何区分中子星和奇异星是当前核天体物理研究中的热点课题。本文对目前区分中子星和奇异星的三种主要方法进行了一些研究。
     一,介质效应及相应的热力学自洽项对奇异星体粘滞系数的影响。考虑介质效应后,我们对奇异夸克物质的热力学方程进行了热力学自洽处理,在压强中发现了一项由夸克的密度相关有效质量引入的压强附加项。它使得奇异夸克物质的体粘滞系数是未考虑热力学自洽的情况的33%,与不考虑介质效应的情况相比增加了1个数量级。
     二,密度依赖口袋模型中的奇异夸克物质的热力学性质。我们主要考察了密度依赖口袋模型中的热力学自洽问题。由于热力学自洽的要求,我们在压强项中给出了一项由密度依赖的口袋常数所引入的压强附加项。该压强附加项使得奇异星的状态方程偏软,相应的奇异星最大质量和半径更接近脉冲星的正则质量。
     三,密度依赖参数对裸奇异星电子气层的影响。我们比较了密度依赖口袋模型的热力学自洽解和非热力学自洽解对裸奇异星电子气层的影响发现,在裸奇异星的表面处,热力学自洽的状态方程对应的内外电场与非热力学自洽的状态方程对应的内外电场相比增加了12-20%。热力学自洽的状态方程对应的电子数密度比非自洽的状态方程对应的电子数密度增加了17-20%。我们还讨论了密度依赖参数对裸奇异星的电子气层的影响。通过比较各种密度依赖参数对电子气层的影响发现,密度依赖参数的选择以及热力学自洽项对距离表面约200费米之内的电子气层结构有影响且在表面处差异最大。不同模型对应的外电场在表面处的差异约为30-50%。
The conjecture that strange quark matter (SQM) may be the true groundstate of the quantum chromodynamics (QCD) vacuum was proposed nearly threedecades ago. The possible existence of strange stars has attracted manyauthors. It was assumed that all pulsars are strange stars which arecomposed of strange quark matter. If this assumption is proven, bulkquarks are found naturely. In this thesis, the following aspects ofstrange stars have been studied.
     Firstly, we have discussed the bulk viscosity of strange stars. Thebulk viscosity of interacting strange quark matter is calculated in thelight of strange quark mass dependent on the reaction rate of u + s <->d + u. Based on this, we rederive the bulk viscosity of interacting strangequark matter. The extra pressure terms comes from the interaction betweenquarks are included. If the temperature is lower than 0.01MeV, our resultsare 50% smaller than the un-consistent one and one order of magnitude morethan the results which do not consider the medium effects. If thetemperature is higher or equal to 0.01 MeV, our results are 30% smallerthe un-consistent one and twice more than the results which do not considerthe medium effects.
     Secondly, we have studied the thermodynamics of strange quark matterwith density dependent bag constant self-consistently in the frameworkof the general ensemble theory and the MIT bag model. In our treatment,an extra pressure term is derived in the expression of pressure. With theadditional term, the zero pressure locates exactly at the lowest energystate, indicating that our treatment is a self-consistently thermodynamictreatment. The self-consistently thermodynamic equations of state (EOS)of strange quark matter in both the normal and color-flavor-locked (CFL) phase are derived. They are both softer than the inconsistent ones.Strange stars in both of the normal and CFL phase have smaller masses andradii in our treatment. It is interesting to find that the energy densityat a star surface in our treatment is much higher than that in theinconsistent treatment for both phases. Consequently, the surfaceproperties and the corresponding observational properties of strangestars in our treatment are different from those in the inconsistenttreatment.
     Finally, we have compared the effects of self-consistent with theunself-consistent results on the electrosphere of a bare strange star indensity denpendent bag model. It is found that the electric field obtainedby the self-consistent EOS is larger than the electric field obtained bythe unself-consistent EOS about 12-20%. The corresponding electron numberdensity increases about 17-20%. Then we discuss the effects of densitydependent parameters on the structure of the electrosphere of a barestrange star. It is found that the main differences in the structures ofthe electroshpere for different parameters lie in 200 fm from the surface.The largest deviations in the electric field between those models areabout 30-50% on the star surface.
引文
[Abramowicz88] Abramowicz M A, Czerny B, Lasota J P, Szuszkiewicz E. Slim accretion disks. Astrophys. J., 1988, 400:245
    [Aguirre97] Aguirre R, Schvellinger M. Density dependence of the MIT bag parameters from the field theory of hadrons. Phys Lett B, 1997,400:245
    [AguirreO3] Aguirre R. Chiral symmetry and strangeness content in nuclear physics parametrized by a medium dependent bag constant. Phys Lett B, 2003, 559:207
    [Aksenov03] Aksenov A G, Milgrom M, Usov V V. Radiation from hot, bare, strange stars. MNRAS, 2003, 343:L69-72
    [Aksenov04] Aksenov A G, Milgrom M, Usov V V. Structure of Pair Winds from Compact Objects with Application to Emission from Hot Bare Strange Stars. Astrophys. J. 2004, 609:363-377
    [Aksenov05] Aksenov A G, Milgrom M, Usov V V. Pair Winds in Schwarzschild Spacetime with Application to Hot Bare Strange Stars. Astrophys. J. 2005, 632:567-575
    [Alford98] Alford M, Rajagopal K, Wilczek F. QCD at finite baryon density: nucleon droplets and color superconductivity. Phys Lett B, 1998, 247:422
    [AlfordOl] Alford M. , Bowers J. A., and Rajagopal K. Crystalline color superconductivity. Phys. Rev. D. 2001, 63:074016
    [Alford04] Alford M, Kouvaris C, Rajagopal K. Gapless Color-Flavor-Locked Quark Matter. Phys. Rev. Lett. 2004, 92:222001
    [Alford08] Alford M, Schmitt A, Rajagopal K, et al. Color superconductivity in dense quark matter. Rev Mod Phys, 2008 80:1455
    [Andersson98] Andersson N. A New class of unstable modes of rotating relativistic stars. Astrophys. J., 1998, 502: 708
    [Artemova96] Arteraova I V, Bjoernsson G, Novikov I D. Modified Newtonian Potentials for the Description of Relativistic Effects in Accretion Disks around Black Holes. ApJ, 1996,461:565
    [Bao08] Bao T, Liu G Z, Zhao E G, Zhu M F. Self-consistently thermodynamic treatment for strange quark matter in the effective mass bag model. Phys. Rev. C. 1987, 35:213.
    [Berger87] Berger M S, Jaffe R L. Radioactivity in strange quark matter. The European Physical Journal A 2008, 38:251-368.
    [Blaschke99] Blaschke D, Grigorian H, Poghosyan G, Roberts C D, Schmidt S. A dynamical, confining model and hot quark stars. Phys. Lett. B. 1999, 450:207.
    [Bowers02] Bowers J. A. and Rajagopal K. Crystallography ,of color superconductivity. Phys. Rev. D. 2002, 66:065002.
    [Burgio02] Burgio G, Baldo M, Sahu P, et al. Maximum mass of neutronstars with a quark core. Phys Lett B,2002, 526:19
    [Casalbuoni04] Casalbuoni R. and Nardulli G. Inhomogeneous superconductivity in condensed matter and QCD. Rev. Mod. Phys. 2004, 76:263
    [Chakrabarty91] Chakrabarty S. Equation of state of strange quark matter and strange star. Phys. Rev. D, 1991, 43:627-630
    [Chakrabarty93] Chakrabarty S. Stability of strange quark matter at T ≠0. Phys. Rev. D, 1993, 48:1409-1417
    [Chakrabarty96] Chakrabarty S. Quark matter in a strong magnetic field. Phys. Rev. D, 1996, 54.: 1306-1316
    [Cheng03] Cheng K S, Harko T. Surface Photon Emissivity of Bare Strange Stars. Astrophys. J, 2003, 596:451
    [Chmaj91] Chmaj T, Haensel P, Slominski W. Photon emissivity of strange matter. Nuclear Physics B- Proceedings Supplements,1991, 24:40-44
    [Cho74]Chodos A, Jaffe R L, Johnson K, Thorne C B, Weisskopf V F. New extended model of hadrons. Phys. Rev. D, 1974, 9:3471
    [Cohen08] Cohen T, McGady D A. Schwinger mechanism revisited. Phys. Rev. D, 2O08, 78:036008
    [Farhi84] Farhi E, Jaffe R L. Strange matter. Phys. Rev. , 1986, D30: 2379
    [Fowler81] Fowler G N, Raha S, Weiner R M. Confinement and phase transitions. Z. Phys. C, 1981,9:271
    [Gross73] Gross D J, Wilczek F. Asymptotically Free Gauge Theories. I. Phys. Rev. 1973, D8:3633 - 3652
    [Gilson93] Gilson E P, Jaffe R L. Asymptotically Free Gauge Theories. I. Phys. Rev. Lett. 1993, 71:332
    [Harko05] Harko T, Cheng K S. Photon Emissivity of the Electrosphere of Bare Strange Stars. Astrophys. J, 2005, 622:1033-1043
    [Harko06] Harko T, Cheng K S. Electron-Positron Pair Production in the Electrosphere of Quark Stars. Astrophys. J, 2006, 643:318
    [Harris04] Harris J W. Summary of Strange Quark Matter 2003 experimental results. J. Phys. G, 2004, 30:S613
    [Heiselberg94] Heiselberg H. Viscosities of quark-gluonplasmas. Phys. Rev. 1994 D49:4739-4750
    [Haensel86] Haensel P, Zdunik J L, Schaefer R, Strange quark stars. Astro. Astrophys. 1986 160:121-128
    [Haensel99] Haensel P, Lasota J P, Zdunik J L. On the minimum period of uniformly rotating neutron stars. Astro. Astrophys. 1999, 344:151
    [He96] He Y B, Gao C S, Li X Q, Chao W Q. Properties of strangelets at finite temperature in the liquid drop model. Phys. Rev. C, 1996, 53: 1903
    [He96a] He Y B, Gao C S, Li X Q, Chao W Q. Cold strangelets formation with finite size effects in high energy heavy-ion collisions. Phys. Rev. C, 1996, 54: 857
    [Hu97] Huang Y, Lu T. Strange stars: how dense can their crust be? Astron. Astrophys, 1997, 325: 189
    [Huang03] Huang M, Shovkovy I. Gapless color superconductivity at zero and at finitetemperature. Nucl. Phys. A, 2003,729:835-863
    [Huang03] Huang M, Shovkovy I. Gapless color superconductivity at zero and at finite temperature. Nucl. Phys. A, 2003,729:835-863
    [Itoh70] ITOH N. Hydrostatic Equilibrium of Hypothetical Quark Stars, Prog. Theor.Phys. (Tokyo), 1970, 44:291
    [Jaikumar04] Jaikumar P, GaleC, Page D, Prakash M. Bremsstrahlung photons from the bare surf ace of a strange quark star. Phys. Rev. D, 2004,70:023004
    [Jaikumar05] Jaikumar P, Gale C, Page D, Prakash M. Distinguishing Bare Quark Stars from Neutron Stars. International Journal of Modern Physics A, 2005, 19:5335-5342
    [Jin96] Jin X M, Jennings B K. Prakash M. Recovering relativistic nuclear phenomenology from the quark-meson coupling model. Phys. Lett. B. 1996, 374:13
    [Jin96a] Jin X M, Jennings B K. Prakash M. Modified quark-meson coupling model for nuclear matter. Phys. Rev. C. 1996, 54:1427
    [Kato95] Kato S, Honma F, Matsumoto R. Pulsational instability of transonic regions of accretion disks with conventional alpha-viscosity. PASJ, 1988, 40:709
    [Kettner95] Kettner C,- Weber F, Weigel M, Glendenning N. Structure and stability of strange and charm stars at finite temperatures. Phys. Rev. D, 1995, 51:1440
    [Landau53] Landau L D, Pomeranchuk I. Limits of applicability of the theory of bremsstrahlung electrons and pair production at high-energies. Dokl. Akad. Nauk Ser. Fiz. ,1953, 92:535
    [Lattimer04] Lattimer J. M., Prakash M. , The Physics of Neutron Stars. Science 2004, 304:536
    [Li09] Li A, Xu R X, Lu J F. Strange stars with different quark mass scalings. Arxiv 2009, 0905:3439vl
    [Li99]LiXD. Is SAX J1808. 4-3658 a Strange Star? Phys. Rev. Lett. 1999, 83:3776
    [Lindblom99] Lindblom L, Mendell G, Owen B J. Second-order rotational effects on the r-modes of neutron stars. Phys. Rev., 1999, D60: 064006
    [Liu0l] Liu Y X, Gao D F, Guo H. Density dependence of nucleon bag constant, radius and mass in an electric field theory model of QCD. Nucl Phys A, 2001, 695:353
    [Lu85] Lu J F. Non-uniqueness of transonic solution for accretion onto a Schwarzschild black hole. Astro. & Astrophys. , 1985, 148:176
    [Lu98] Lu D H, Tsushima K, Thomas A W, Williams A G, Saito, K. Medium dependence of the bag constant in the quark-meson coupling model. Nucl Phys A, 1998, 634:443
    [Madsen92] Madsen J. Bulk viscosity of strange quark matter, damping of quark star vibration, and the maximum rotation rate of pulsars. Phys. Rev., 1992, D46: 3290
    [Madsen93] Madsen J. Rate of the weak reaction s+u—u+d in quark matter. Phys. Rev. 1993, D47: 325
    [Madsen93a] Madsen J. Curvature contribution to the mass of strangelets. Phys. Rev. Lett, 1993, 70:391
    [Madsen93b] Madsen J. Mass formula for strange and nonstrange quark matter. Phys. Rev. 1993, D47: 5156
    [Madsen94] Madsen J. Shell model versus liquid drop model for strangelets. Phys.' Rev. D, 1994, 50:3328
    [Madsen98] Madsen J. How to identify a strange star. ' Phys. Rev. Lett., 1998, 81: 3311
    [MadsenOO] Madsen J. Probing Strange Stars and Color Superconductivity by r-Mode Instabilities in Millisecond Pulsars. Phys. Rev. Lett., 2000, 85: 10-13
    [MadsenOOa] Madsen J. Intermediate Mass Strangelets are Positively Charged. Phys. Rev. Lett., 2000, 85: 4687
    [MadsenOl] Madsen J. Color-Flavor Locked Strangelets. Phys. Rev. Lett. , 2001, 87: 172003
    [Matsumoto84] Matsumoto R, Kato S, Fukue J, Okazaki A T. Viscous transonic flow around the inner edge of geometrically thin accretion disks. PASJ,1984, 36:71-85
    [Migdal56] Migdal A B. Bremsstrahlung and Pair Production in Condensed Media at High Energies. Phys. Rev, 1956, 103:1811
    [Muchotrzeb81] Muchotrzeb B, Paczynski B. Transonic accretion flow in a thin disk around a black hole. Acta Astronomica. 1982, 32:1-11.
    [Muller81] Muller B, Rafelski J. Temperature dependence of the bag constant and the elective lagrangian for gauge fields at finite temperatures. Phys Lett B,1981,101:111
    [Muller97].Muller H, Jennings, B K. Nuclear matter properties of the modified quark-meson coupling model. Nucl. Phys. A. 1997, 626:966
    [Nikishov70] Nikishov A. Barrier scattering in field theory removal of Klein paradox. Nucl. Phys. B, 1970,21:346
    [Nikishov89] Novikov I D, Frolov V P. Physics of black holes ((Fizika chernykh dyr, Moscow, Izdatel*stvo Nauka, 1986, 328 p) Dordrecht, Netherlands, Kluwer Academic Publishers, 1989, 351 p. Translation.)
    [Nowak91] Nowak M A, Wagoner R V. Diskoseismology: Probing accretion disks. I - Trapped adiabatic oscillations. Astrophys. J 1991, 378:656
    [0pp39] OPPENHEIMER J R, VOLKOFF G M. On massive neutron cores. Phys. Rev., 1939, 55:374-381
    [Paczynski80] Paczynsky, B. ; Wiita," P. J. Thick accretion disks and supercritical luminosities. Astro. & Astrophys., 1980, 88:23
    [Page02] Page D, Usov V. 2002, Thermal Evolution and Light Curves of Young Bare Strange Stars. Phys. Rev. Lett., 2002, 89:131101
    [Parjia93] Parija B C. Dynamical effects of quantum chromodynamics on the surface tension of a cold strange quark nugget. Phys. Rev. C, 1993, 48:2483
    [Parjia95] Parija B C. Collective modes in a strangelet. Phys. Rev. C, 1995, 51:1473
    [PengOO] Peng G X, Chiang H C, Zou B S et al. Thermodynamics, strange quark matter, and strange stars. Phys. Rev., 2000, C62:025801
    [Peng06] PENG G X, WEN X J, CHEN Y D. New solutions for the color-flavor locked strangelets. Phys. Lett., 2006, 3633:314-318
    [Peng08] PENG G X, Li A, Lombardo U. Deconfinement phase transition in hybrid neutron stars from the Brueckner theory with three-body forces and a quark model with chiral mass scaling. Phys. Rev., 2008, C77:065807
    [Politzer73] Politzer H D. Reliable Perturbative Results for Strong Interactions? Phys. Rev. Lett., 1973, 30:1346-1349
    [Reinhardt86] Reinhardt H, Dang B V. Dynamical bag constant and surface tension of baryon droplets at finite temperature and density. Phys Lett B, 1986, 173:473
    [Ratti03] Ratti C. The NJL model and strange-quark matter. Europhys. Lett, 2003, 61:314
    [Sawyer89] Sawyer R S. Damping of vibrations and of the secular instability in quark stars. Phys. Lett., 1989, B233: 412
    [Schanffner97] Schaffner-Bielich J, Greiner C, Diener A, Stocker H. Detectability of strange matter in heavy ion experiments. Phys. Rev. C, 1997, 55: 3038
    [Schafer97] Schafer T. The ground state of strange quark matter. Nucl. Phys. A, 2002, 702:167
    [Schertler97] Schertler K, Greiner C, Thoma M H. Medium effects in strange quark matter and strange stars. Nucl. Phys. , 1997, A616: 659-679
    [Schertler98] Schertler K, Greiner C, Sahu P K, Thoma M H. The influence of medium effects on the gross structure of hybrid stars. Nucl. Phys. , 1997, A637: 451-465
    [SchertlerOO] Schertler K, Greiner C, Schaner-Bielich J et al. Quark phases in neutron stars and a third family of compact stars as signature for phase transitions. Nucl. Phys., 2000, A677: 463-490
    [Shovkovy03] Shovkovy I, Huang M. Gapless two-flavor color superconductor. Phys. Lett. B 2003,564:205
    [Schwinger51] Schwinger J. On Gauge Invariance and Vacuum Polarization. Phys. Rev.,1951, 82:664
    [Tolman39] TOLMAN R C. Static solutions of Einstein' s field equation for spheres of fluid. Phys. Rev., 1939, 55:364-373
    [Usov98] Usov V V. Bare Quark Matter Surfaces of Strange Stars and eV Emission. Phys. Rev. Lett., 1998, 80:230
    [UsovOl] Usov V V. Strange Star Heating Events as a Model for Giant Flares of Soft-Gamma-Ray Repeaters. Phys. Rev. Lett. 2001, 87:021101
    [Usov04] Usov V V. Electric fields at the quark surface of strange stars in the color-flavor locked phase. Phys. Rev. D, 2004, 70:067301
    [Usov05] Usov V V, Harko T, Cheng K S: Structure of the Electrospheres of Bare Strange Stars. Astrophys. J, 2005, 620:915-921
    [Wang84] Wang Q D, LU T. The damping effects of the vibrations in the core of a neutron star. Phys. Lett., 1984, B148: 211
    [ffang03] Wang P, Lyubovitskij V E, Gutsche T, Faessler, A. Strange quark matter in a chiral SU(3) quark mean field model. Phys. Rev. C, 2003, 67:015210
    [Witten84] WittenE. Cosmic separation of phases. Phys. Rev., 1984, D30: 272
    [Web05] WEBER F. Strange quark matter and compact stars. Prog. Part. Nucl. Phys. , 2005, 54:193-288
    [Wen07] Wen X J, Peng G X, Chen Y D. Charge, strangeness and radius of strangelets. Journal of Physics G: Nuclear and Particle Physics, 2007, 34:1697-1709
    [Xu02] Xu R X. A THERMAL FEATURELESS SPECTRUM: EVIDENCE FOR BARE STRANGE STARS? The Astrophysical Journal, 2002, 570:L65-L68
    [ZhangOO] Zhang B, Xu R X, Qiao G J. Nature and Nurture: a Model for Soft Gamma-Ray Repeaters. Astrophys. J, 2000, 545:L127
    [Zdunik02] Zdunik J L. On the minimum radius of strange stars with crust. Astro. Astrophys. 2002,394:641
    [Zheng02] Zheng X P, Yang S H, Li J R et al. Bulk viscosity of interacting strange quark matter. Phys. Lett., 2002,B548: 29
    [Zheng04] Zheng X. P., Liu X. W, Kang M. et al. Bulk viscosity of strange quark matter in a density-dependent quark mass model and dissipation of the r mode in strange stars. Phys. Rev., 200

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