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arXiv 2304.03329astro-ph.HEastro-ph.SR
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强磁化恒星周围的双温吸积流及其光谱分析

Two-temperature accretion flows around strongly magnetized stars and their spectral analysis

Shilpa Sarkar, Kuldeep Singh, Indranil Chattopadhyay, Philippe Laurent

AI总结:

本文研究强磁化致密星周围的双温吸积流,通过熵最大原则选定唯一跨声速解,并分析主激波与次激波对光谱的贡献,发现次激波会在高能段产生扩展发射。

摘要:

我们研究了强磁化致密星周围的双温吸积流。物质以吸积盘形式被吸积至盘半径($r_{\rm d}$)处,在该处磁压超过气压和冲压,此后物质沿磁力线被引导到磁极上。我们沿磁力线自洽地求解运动方程,并纳入韧致辐射、同步辐射和逆康普顿化等辐射过程。对于给定的一组运动常数,运动方程并不产生唯一的跨声速解。根据热力学第二定律,选择熵最高的解,从而消除了解的简并性。我们研究了这些解的性质,并获得了相应的光谱,作为磁场($B_*$)、自转周期($P$)和恒星吸积率($\dot{M}$)的函数。主激波总是在表面附近形成。该激波后区域中增强的辐射过程使物质减速,最终沉降在恒星表面。该激波后区域贡献了吸积流总光度的$\gtrsim 99.99\\%$。研究完整吸积流仍然很重要,因为对于某些$B_*$、$P$和${\dot{M}}$的组合,除主激波外还可能存在次激波。我们发现,如果存在次激波,它们会在光谱的更高能量处产生扩展发射。

英文摘要:

We investigate two-temperature accretion flows onto strongly magnetized compact stars. Matter is accreted in the form of an accretion disc upto the disc radius ($r_{\rm d}$), where, the magnetic pressure exceeds both the gas and ram pressure and thereafter the matter is channelled along the field lines onto the poles. We solve the equations of motion self-consistently along the field lines, incorporating radiative processes like bremsstrahlung, synchrotron and inverse-Comptonization. For a given set of constants of motion, the equations of motion do not produce unique transonic solution. Following the second law of thermodynamics the solution with the highest entropy is selected and thereby eliminating the degeneracy in solution. We study the properties of these solutions and obtain corresponding spectra as a function of the magnetic field ($B_*$), spin period ($P$) and accretion rate of the star ($\dot{M}$). A primary shock is always formed just near the surface. The enhanced radiative processes in this post-shock region slows down the matter and it finally settles on the surface of the star. This post-shock region contributes to $\gtrsim 99.99\%$ of the total luminosity obtained from the accretion flow. It is still important to study the full accretion flow because secondary shocks may be present for some combination of $B_*$, $P$ and ${\dot{M}}$ in addition to primary shocks. We find that secondary shocks, if present, produce an extended emission at higher energies in the spectra.

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