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arXiv 1505.03255astro-ph.SR
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磁化中子星的差旋和r模

Differential rotation and r-modes in magnetized neutron stars

Andrey I. Chugunov

摘要:

Rezzolla等人[ApJ 531(2000),L139; Phys. Rev. D 64(2001),104013; Phys. Rev. D 64(2001),104014]将注意力集中在与r模相关的二阶长期漂移上,并声称它会导致磁场增强和磁化中子星中r模不稳定性的抑制。我们批判性地修正了这些结果。我们提出了一个特殊的二阶r-模式的解决方案与消失的长期漂移,从而驳斥了一个广泛认为的声明,长期漂移是一个不可避免的功能的r-模式。如果$B\ll B_{\mathrm{crit}}\approx 10^{17}\,(ν/600\,\mathrm{Hz})$ G($ν$是自旋频率),则该非漂移解不受磁场$B$的影响,并且不导致磁场的长期演化。对于一般的二阶r模解,漂移不一定为零,但可以表示为两个解的叠加:一个描述非振荡星的微分转动演化(描述长期漂移;对于非磁化星,它是圆柱上分层的任意定常旋转;磁化星的微分自转在Alfvén时间尺度上演化,并可能导致磁能增强),另一种是上述的非漂移r模解。这种表示使我们能够得出结论,磁场能量的增强受到差分旋转的初始能量的限制,该初始能量比r模式的总能量小得多(对于因子$\propto α^2$,其中$α$是模式振幅)。因此,由漂移引起的磁场增强不能抑制r模式不稳定性。结果可以推广到任何介质中的任何振荡模式,如果该模式具有$B=0$的非漂移解。

英文摘要:

Rezzolla et al. [ApJ 531 (2000), L139; Phys. Rev. D 64 (2001), 104013; Phys. Rev. D 64 (2001), 104014] draw attention to the second order secular drift associated with r-modes and claimed that it should lead to magnetic field enhancement and suppression of r-mode instability in magnetized neutron stars. We critically revise these results. We present a particular second order r-mode solution with vanishing secular drift, thus refuting a widely believed statement that secular drift is an unavoidable feature of r-modes. This non-drifting solution is not affected by magnetic field $B$, if $B\ll B_{\mathrm{crit}}\approx 10^{17}\,(ν/600\,\mathrm{Hz})$ G ($ν$ is a spin frequency) and does not lead to secular evolution of magnetic field. For general second order r-mode solution the drift does not necessarily vanish, but the solution can be presented as a superposition of two solutions: one describes evolution of differential rotation in nonoscillating star (which describes secular drift; for nonmagnetized star it is arbitrary stationary rotation stratified on cylinders; for magnetized star differential rotation evolves on the Alfvén timescale and may lead to magnetic energy enhancement), and another one is non-drifting r-mode solution mentioned above. This representation allows us to conclude that enhancement of magnetic field energy is limited by initial energy of differential rotation, which is much less (for a factor $\propto α^2$, where $α$ is mode amplitude) than the total energy of r-mode. Hence, magnetic field enhancement by drift cannot suppress r-mode instability. Results can be generalized for any oscillation mode in any medium, if this mode has non-drifting solution for $B=0$.

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