用中子星弓形冲击探测非辐射冲击的低速区

Stella Koch Ocker and Maren Cosens
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摘要

非辐射冲击会加速粒子并加热天体物理等离子体。超新星残骸是研究最深入的例子,而中子星(NS)的弓形冲击也是非辐射性的,并且以巴尔默(Balmer)为主。中子星弓形冲击由于其诞生时的巨大速度,在星际介质中可能无处不在,而且它们被认为是对银河宇宙射线频谱有贡献的离散源群。迄今为止,已经在 Hα 图像中直接观测到九个 NS 弓形冲击。这些冲击大多是通过窄带 Hα 成像和狭缝光谱来描述的,无法解析冲击的多分量速度结构及其空间几何形状。在这里,我们展示了三个 NS 弓形冲击的积分场光谱:J0742-2822、J1741-2054和J2225+6535(吉他星云)。我们从四个维度同时测量了冲击的特性:二维投影冲击形态、径向速度结构和Hα通量。根据径向速度剖面推断出宽窄线比率(Ib/In),对于J1741-2054,在冲击的多个区域都探测到了窄线。推断出的线比和宽度表明,NS弓形冲击代表了一种低冲击速度机制(V ≲ 200 km s-1),在这种机制中,Ib/In很高,与超新星残余物探测到的冲击机制不同。我们的研究结果表明,有必要在比以前考虑的速度更低的速度下建立非辐射冲击模型,这将揭示这些弓形冲击的电子-离子温度比和粒子加速效率。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Probing the Low-velocity Regime of Nonradiative Shocks with Neutron Star Bow Shocks
Nonradiative shocks accelerate particles and heat astrophysical plasmas. While supernova remnants are the most well-studied example, neutron star (NS) bow shocks are also nonradiative and Balmer dominated. NS bow shocks are likely ubiquitous in the interstellar medium due to their large speeds imparted at birth, and they are thought to be a discrete source population contributing to the Galactic cosmic-ray spectrum. To date, nine NS bow shocks have been directly observed in Hα images. Most of these shocks have been characterized using narrowband Hα imaging and slit spectroscopy, which do not resolve the multicomponent velocity structure of the shocks and their spatial geometry. Here we present integral field spectroscopy of three NS bow shocks: J0742−2822, J1741−2054, and J2225+6535 (the Guitar Nebula). We measure the shock properties simultaneously in four dimensions: the 2D projected shock morphology, the radial velocity structure, and the Hα flux. The broad-to-narrow line ratio (Ib/In) is inferred from radial velocity profiles, and for J1741−2054, the narrow line is detected in multiple regions of the shock. The inferred line ratios and widths suggest that NS bow shocks represent a low-shock velocity regime (V ≲ 200 km s−1) in which Ib/In is high, distinct from the shock regime probed by supernova remnants. Our results illustrate a need for nonradiative shock models at velocities lower than previously considered, which will reveal the electron–ion temperature ratios and particle acceleration efficiencies of these bow shocks.
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