数理化科学

中子星辐射引力红移的量子真空极化修正

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  • 1. 上海大学理学院, 上海200444; 2. 上海市天体物理重点实验室, 上海200234

收稿日期: 2012-04-26

  网络出版日期: 2013-04-30

基金资助

上海市自然科学基金资助项目(09ZR1410900)

Quantum Vacuum Polarization Modification for Gravitational Redshift of Neutron Star Emissions

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  • 1. College of Sciences, Shanghai University, Shanghai 200444, China; 2. The Shanghai Key Laboratory of Astrophysics, Shanghai 200234, China

Received date: 2012-04-26

  Online published: 2013-04-30

摘要

测量中子星表面辐射谱的引力红移被认为是探究这类致密天体基本物理特性最为直接有效的手段. 但是,脉冲星、磁星这些强磁化中子星表面的辐射红移不仅源于引力的作用, 还需要考虑星体表面的磁化等离子体以及由超强磁场所诱导的量子电动力学(quantum electrodynamics, QED) 真空极化效应对辐射的电磁作用. 运用Gordon有效度规理论研究磁化等离子体以及QED真空极化效应对星体辐射的影响. 计算结果表明, 一般情况下对辐射引力红移的修正起主要作用的是星体表面的磁化等离子体, 但在某些特定情况下, 还必须考虑QED真空极化效应的作用.

本文引用格式

陈家麟1, 季沛勇1,2 . 中子星辐射引力红移的量子真空极化修正[J]. 上海大学学报(自然科学版), 2013 , 19(2) : 176 -180 . DOI: 10.3969/j.issn.1007-2861.2013.02.013

Abstract

Measuring the gravitational redshift of neutron star emission lines is the most effective and feasible method for determining fundamental properties of these compact objects. It is found that redshift of emission lines of pulsars and magnetars is produced not only by the gravitational field but also by surface magnetoplasma and quantum electrodynamics (QED) vacuum polarization effect induced by the super-strong magnetic field.The effect on the stellar emission caused by magnetoplasma and quantum vacuum polarization is studied within the framework of Gordon’s effective metric theory. It is shown that modification of gravitational redshift is mainly caused by magnetoplasma, and contributions of the QED vacuum polarization effect should also be
taken into account in some particular cases.

参考文献

[1] Lattimer J M. Neutron star equation of state [J]. New Astronomy Reviews, 2010, 54(3/4/5/6): 101-109.
[2] Tr¨umper J. X-ray observations of neutron stars and the equation of state at supra-nuclear densities [J]. New Astronomy Reviews, 2010, 54(3/4/5/6): 122-27.

[3] Zhang C M, Yin H X, Kojima Y, et al. Measuring neutron star mass and radius with three mass-radius relations [J]. Mon Not R Astron Soc, 2007, 374(1): 232-236.

[4] Cottam J, Paerls F, Mendez M. Gravitationally redshifted absorption lines in the X-ray burst spectra of a neutron star [J]. Nature, 2002, 420(6911): 51-64.

[5] Harding A K, Lai D. Physics of strongly magnetized neutron stars [J]. Rep Prog Phys, 2006, 69(9): 2631-2708.

[6] Zhu J, Ji P Y. Modification of gravitational redshift of X-ray burst produced by pulsar surface magnetoplasma [J]. Chin Phys B, 2007, 17(1): 356-361.

[7] Ji P Y, Qu S W, Bai Y. Modified surface redshift of pulsars produced by magnetoplasma [J]. Gen Relativ Gravit, 2008, 40(1): 131-138.

[8] Brodin G, Marklund M, Stenflo L, et al. Dispersion relation for electromagnetic wave propagation in a strongly magnetized plasma [J]. New J Phys, 2006, 8(16): 16-21.

[9] Bu Z G, Ji P Y. Quantum electrodynamics vacuum polarization modification of photon acceleration in plasma [J]. Phys Plasmas, 2010, 17(7): 1-6.

[10] Gordon W. Zur lichtfortpflanzung nach der relativit¨atstheorie [J]. Ann Phys, 1923, 72(22): 421-456.

[11] Misner C W, Thorne K S, Wheeler J A. Gravitation [M]. San Francisco: Freeman, 1973: 657-659.

[12] 季沛勇. Einstein 引力理论在激光-等离子体相互作用中的应用[D]. 上海: 上海大学, 2006: 50-68.

[13] Melrose D B. Pulsar emissions [J]. Plasma Phys Control Fusion, 2003, 45(5): 523-534.

[14] Kramer M, Stappers B W, Jessner A, et al. Polarized radio emission from a magnetar [J]. Mon Not R Astron Soc, 2007, 377(1): 107-119.

[15] Lundin J, Steno L, Brodin G, et al. Circularly polarized waves in a plasma with vacuum polarization effects [J]. Phys Plasmas, 2007, 14(6): 1-3.

[16] Goldreich P, Julian W. Pulsar electrodynamics [J]. Astrophys J, 1969, 157: 869-880.

[17] Gedalin M, Melrose D B. Long waves in a relativistic pair plasma in a strong magnetic field [J]. Phys Rev E, 1998, 57(3): 3399-3410.

[18] Duncan R C, Thompson C. Formation of very strongly magnetized neutron stars-implications for gamma-ray bursts [J]. Astrophys J, 1992, 392(1): 9-13.

[19] Camilo F, Ransom S M, Halpern J P, et al. A radio-emitting magnetar with a rotation period of 2 seconds [J]. Astrophys J, 2007, 666(2): 93-96.
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