论文标题

围绕SGR A*:简单$χ^2 $分析光子从绕恒星红移的限制

Constraints on the dark mass distribution surrounding Sgr A*: simple $χ^2$ analysis for the redshift of photons from orbiting stars

论文作者

Takamori, Yohsuke, Nishiyama, Shogo, Ohgami, Takayuki, Saida, Hiromi, Saitou, Rio, Takahashi, Masaaki

论文摘要

Sagittarius A*(Sgr a*)是质量$ \ sim 4 \ sim 4 \ sim 10^6 m _ {\ odot} $的中央超级黑洞,并以银河系为单位,而恒星则围绕它绕。 2018年5月,最接近SGR A*名为S0-2/S2的恒星之一经历了周围的通道。来自S0-2的光子的红移从$ 4000 \> {\ rm km \> s^{ - 1}} $到$ -2000 \> {\ rm km \> s^{ - 1}} $ {\ rm km \> s^{ - 1}} $,在周围通行证中,在$ 0.5 \ \> \ rm yr}内。在本文中,我们表明,红移的这种陡峭变化对S0-2轨道内的深色质量分布有很大的限制。通过将简单的$χ^2 $分析应用于观察到的红移,我们可以轻松区分两个模型,点质量模型和点质量质量和扩展的质量模型,而无需最佳拟合参数搜索。我们的红移数据在2018年的候选器段落期间,Subaru/ircs限制了S0-2内部的延长质量的数量小于$ 0.5 \,\%$($ \ sim 2 \ times 10^4 m_ \ odot $)sgr a*的质量。通过我们的简单分析获得的这种约束与以前的作品相媲美,最合适的参数搜索与S0-2运动的运动,包括扩展质量的效果。我们考虑了深色质量分布模型的幂律和掉线模型,但是找不到这些结果之间的显着差异。

Sagittarius A* (Sgr A*) is the central supermassive black hole with the mass $\sim 4\times 10^6 M_{\odot}$ in the Milky Way and stars are orbiting around it. In May 2018, one of the nearest stars to Sgr A* named S0-2/S2 experienced the pericenter passage. The redshift of photons from S0-2 had varied from $4000\>{\rm km\>s^{-1}}$ to $-2000\>{\rm km\>s^{-1}}$ during the pericenter passage, which is within $0.5\>{\rm yr}$. In this paper, we show that this steep variation of the redshift gives a strong constraint on a dark mass distribution inside the orbit of S0-2. By applying a simple $χ^2$ analysis to the observed redshift, we can easily distinguish between the two models, the point mass model and the point mass plus an extended mass model without the best-fitting parameter search. Our redshift data during the pericenter passage in 2018 with Subaru/IRCS bound the amount of the extended mass inside the orbit of S0-2 less than $0.5\,\%$ ($\sim 2 \times 10^4 M_\odot$) of the mass of Sgr A*. This constraint obtained by our simple analysis is comparable to previous works with the best-fitting parameter search to the motion of S0-2 including the effect of the extended mass. We consider both the power-law and the Plummer models for the dark mass distribution model, but the significant difference between these results is not found.

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