经典新星的多频行为

黄金时代 Pub Date : 2018-06-06 DOI:10.22323/1.315.0047
I. Hachisu, M. Kato
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引用次数: 0

摘要

我们回顾了我们目前对经典新星和循环新星的多波长光曲线的理解,并展示了如何确定WD质量和其他双星特性。我们选取了PW Vul, U Sco, V745 Sco, RS Oph和V407 Cyg作为不同类型光曲线的代表,详细研究了它们的光曲线,讨论了它们的物理性质,并阐明了这些差异的原因。在上升阶段,富氢包层扩展到一个紧密的双星的大小之外,其中的伴星被深嵌在光球的内部。在光学最大值之后,伪光球开始收缩,在光球外形成一个光学薄区。在相对较长的波长(光学和近红外)处,自由-自由发射占主导地位,其光曲线沿$F_\nu \propto t^{-1.75}$(或$t^{-1.55}$)的普遍衰减规律衰减。提出了超爱丁顿相的物理机理。在抛射物和星周物质之间存在激波相互作用的情况下,它减缓了光通量的衰减,如$F_\nu \propto t^{-1.0}$所见,在V407 Cyg的早期阶段。在爆发的最后阶段,风的质量损失率急剧下降,使自由-自由发射的斜率衰减,如$F_\nu \propto t^{-3.5}$。超软x射线阶段开始并持续到氢核燃烧结束,之后新星进入冷却阶段。硬x射线可能来自弹射体之间的内部激波(或弹射体与伴星之间的弓形激波)。光优势相、紫外优势相和超软x射线源相的行为对WD质量和包膜化学成分有不同的依赖关系,因此多波长观测有助于确定WD质量等参数。最后,我们应该注意到新星爆发的早期阶段仍未被探索。理论上已经确定了x射线闪光相位,但尚未成功检测到。对早期x射线闪光的探测提供了关于热核失控的直接信息。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Multifrequency behavior of classical novae
We review our current understanding of multiwavelength light curves of classical and recurrent novae and show how to determine the WD masses and other binary properties. We pick up PW Vul, U Sco, V745 Sco, RS Oph, and V407 Cyg as representatives of different types of light curves, examine their light curves in detail, discuss physical properties, and clarify the reason of these differences. In the rising phase, the hydrogen-rich envelope expands beyond the size of a close binary in which the companion is embedded deep inside of the photosphere. After the optical maximum, the pseud-photosphere begins to shrink and an optically thin region develops outside of the photosphere. The free-free emission dominates the flux at relatively longer wavelengths (optical and NIR), of which light curves decay along the universal decline law of $F_\nu \propto t^{-1.75}$ (or $t^{-1.55}$). The physical mechanism of super-Eddington phase is presented. In the presence of shock interaction between ejecta and circumstellar matter, it slows down the decay of optical flux as $F_\nu \propto t^{-1.0}$ as seen in the early phase of V407 Cyg. In final stages of outbursts, the wind mass-loss rate sharply drops so the slope of free-free emission decays like $F_\nu \propto t^{-3.5}$. Supersoft X-ray phase begins and continues until hydrogen nuclear burning ends, and after that the nova enters a cooling phase. Hard X-rays may originate from internal shocks between ejecta (or a bow shock between ejecta and the companion). The behaviors of optical-dominant, UV-dominant, and supersoft X-ray source phase have different dependences on the WD mass and envelope chemical composition, so multiwavelength observations are useful to determine the parameters such as the WD mass. Finally, we should note that the very early phase of nova outbursts remains unexplored. An X-ray flash phase is theoretically identified, but not yet successfully detected. Detections of early X-ray flashes give direct information on thermonuclear runaway.
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