【24h】

Electrodynamics of neutron stars [Review]

机译:中子星的电动力学[综述]

获取原文
           

摘要

Although the standard model for radio pulsars is a rotating magnetized neutron star and the vast majority (if not all) of pulsars are thought to have appreciable inclination angles between the spin and magnetization axes, most theoretical papers use simplified held models (e.g., aligned spin axis and magnetic dipole axis). Deutsch long ago gave exact tin vacuo) closed expressions for these inclined fields (modulo some typos and oversights), but these expressions were rather clumsy and required extensive hand processing to convert into ordinary functions of radius and angle for the electromagnetic fields. Moreover, these expressions were effectively written down by inspection (no details of the derivations given), which leaves the reader with little physical understanding of where the various electric and magnetic held components come from, particularly near the neutron star surface where many models assume the radio emission is generated. Finally, rather little analysis of what these fields implied was given beyond speculation that they could accelerate cosmic rays. As pulsar models become more sophisticated, it seems important that all researchers use a consistent set of underlying fields, which we hope to present here, as well as understand why these fields are present. It is also interesting to know what happens to charged particles from the star that move in these fields. Close to the star, ambient particles tend to simply E x B drift around the star with the same rotational velocity as the star itself. But far from the star, charged particles are accelerated away in the wave zone, as was first pointed out by Ostriker and Gunn. We expand their calculations using more general fields and elucidate the particle's dynamics accordingly. Very efficient acceleration is observed even for particles starting at > 10(3) light-cylinder distances. We also stress the effects of a non-zero radial magnetic field. Electrons are accelerated to much higher energies than, say, protons (not to the same energy as when the two cross a fixed potential drop). We pay particular attention to particles accelerated along the spin axis (particles that might be involved in jet formation). An important limitation to the present work is the neglect of collective radiation reaction. Single particle radiation reaction (e.g., Compton scattering of the wave flux) is not an accurate estimate of the forces on a plasma. We are working on remedying this limitation. (C) 1999 Elsevier Science B.V. All rights reserved. [References: 37]
机译:尽管无线电脉冲星的标准模型是旋转的磁化中子星,并且绝大多数(如果不是全部)脉冲星被认为在自旋轴和磁化轴之间具有明显的倾斜角,但是大多数理论论文都使用简化的保持模型(例如,对准的自旋)轴和磁偶极轴)。 Deutsch很久以前就给出了这些倾斜磁场的精确闭口表达式(对一些错别字和疏忽进行了模数化),但是这些表达式相当笨拙,需要大量的手工处理才能转换成电磁场的半径和角度的普通函数。此外,这些表达式是通过检查有效地写下的(未提供派生的详细信息),这使读者对各种电和磁保持成分的来源(特别是在许多模型假定为中子星表面附近)的物理理解很少。产生无线电发射。最后,除了推测它们会加速宇宙射线外,对这些场的含义的分析很少。随着脉冲星模型变得越来越复杂,所有研究人员都必须使用一组一致的基础场,这一点很重要,我们希望在此处介绍这些场,以及理解为什么存在这些场。知道在这些场中移动的恒星带电粒子发生了什么也很有趣。靠近恒星,环境粒子趋于简单地以与恒星本身相同的旋转速度使E x B在恒星周围漂移。但是,正如Ostriker和Gunn最初指出的那样,带电粒子在远离恒星的地方被加速离开了波带。我们使用更一般的字段扩展它们的计算,并相应地阐明粒子的动力学。即使对于大于10(3)光柱距离的粒子,也可以观察到非常有效的加速。我们还强调了非零径向磁场的影响。电子被加速到比质子高得多的能量(而不是与质子穿过固定电位降时的能量相同)。我们特别注意沿自旋轴加速的粒子(可能与射流形成有关的粒子)。当前工作的一个重要局限是对集体辐射反应的忽视。单粒子辐射反应(例如波通量的康普顿散射)不是对等离子体上力的准确估计。我们正在努力纠正此限制。 (C)1999 Elsevier Science B.V.保留所有权利。 [参考:37]

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号