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Dynamical onset of superconductivity and retention of magnetic fields in cooling neutron stars

机译:冷却中子恒星磁场超导和磁场保持动态发作

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摘要

Asuperconductor of paired protons is thought to form in the core of neutron stars soon after their birth. Minimum energy conditions suggest magnetic flux is expelled from the superconducting region due to the Meissner effect, such that the neutron star core is largely devoid of magnetic fields for some nuclear equation of state and proton pairing models. We show via neutron star cooling simulations that the superconducting region expands faster than flux is expected to be expelled because cooling timescales are much shorter than timescales of magnetic field diffusion. Thus magnetic fields remain in the bulk of the neutron star core for at least 10~6–10~7 yr. We estimate the size of flux free regions at 10~7 yr to be approx<100 m for a magnetic field of 10~(11) G and possibly smaller for stronger field strengths. For proton pairing models that are narrow, magnetic flux may be completely expelled from a thin shell of approximately the above size after 10~5 yr. This shell may insulate lower conductivity outer layers, where magnetic fields can diffuse and decay faster, from fields maintained in the highly conducting deep core.
机译:成对质子的asupercormon被认为在他们出生后不久的中子恒星的核心形成。最小能量条件表明由于凸起的效应,从超导区域排出磁通量,使得中子星芯主要没有用于某些状态和质子配对模型的某些核方程的磁场。我们通过中子星冷却模拟显示超导区域的速度比磁通快,因为冷却时间数比磁场扩散的时间数短得多。因此,磁场留在中子星芯的体积至少10〜6-10〜7之间。我们估计10〜7的磁通区域的尺寸约为10〜(11)克的磁场大约<100μm,并且可能更小的用于更强的场强。对于窄的质子配对模型,磁通量可以在10〜5年后从大约上述尺寸的薄壳体完全排出。该壳体可以绝缘下部导电性外层,其中磁场可以弥漫和衰减更快,从保持在高导电的深核心。

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  • 来源
    《Physical Review C》 |2017年第2017期|065801.1-065801.6|共6页
  • 作者单位

    Mathematical Sciences and STAG Research Centre University of Southampton Southampton SO17 1BJ United Kingdom Physics and Astronomy University of Southampton Southampton SO17 1BJ United Kingdom;

    Mathematical Sciences and STAG Research Centre University of Southampton Southampton SO17 1BJ United Kingdom;

    Department of Physics and McGill Space Institute McGill University Montreal Quebec H3A 2T8 Canada;

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