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A Stellar Wind Origin for the G2 Cloud: Three-Dimensional Numerical Simulations

机译:G2云的恒星风起源:三维数值   模拟

摘要

We present 3D, adaptive mesh refinement simulations of G2, a cloud of gasmoving in a highly eccentric orbit towards the galactic center. We assume thatG2 originates from a stellar wind interacting with the environment of the SgrA* black hole. The stellar wind forms a cometary bubble which becomesincreasingly elongated as the star approaches periastron. A few months afterperiastron passage, streams of material begin to accrete on the central blackhole with accretion rates $\dot{M} \sim 10^{-8}$ M$_\odot$ yr$^{-1}$. PredictedBr$\gamma$ emission maps and position-velocity diagrams show an elongatedemission resembling recent observations of G2. A large increase in luminosityis predicted by the emission coming from the shocked wind region duringperiastron passage. The observations, showing a constant Br$\gamma$ luminosity,remain puzzling, and are explained here assuming that the emission is dominatedby the free-wind region. The observed Br$\gamma$ luminosity ($\sim 8 \times10^{30}$ erg s$^{-1}$) is reproduced by a model with a $v_w=50$ km s$^{-1}$wind velocity and a $10^{-7}$ M$_\odot$ yr$^{-1}$ mass loss rate if theemission comes from the shocked wind. A faster and less dense wind reproducesthe Br$\gamma$ luminosity if the emission comes from the inner, free windregion. The extended cometary wind bubble, largely destroyed by the tidalinteraction with the black hole, reforms a few years after periastron passage.As a result, the Br$\gamma$ emission is more compact after periastron passage.
机译:我们提出了G2的3D自适应网格细化模拟,G2是朝着银河系中心的高偏心轨道中的气体运动云。我们假设G2来自与SgrA *黑洞环境相互作用的恒星风。恒星风形成彗星气泡,随着恒星接近星际星体,彗星气泡变得越来越长。加速器通过后的几个月,物质流开始在中央黑洞上积聚,积聚速率为$ \ dot {M} \ sim 10 ^ {-8} $ M $ _ \ odot $ yr $ ^ {-1} $。预测的Br \γ排放图和位置速度图显示了类似于G2近期观测的细长排放。辉光通过过程中来自风场的辐射预测了光度的大幅增加。观测值显示出恒定的Br \γ亮度,仍然令人费解,在此假设辐射由自由风区控制的情况下进行解释。观测到的Br $ \ gamma $光度($ \ sim 8 \ times10 ^ {30} $ erg s $ ^ {-1} $)由$ v_w = 50 $ km s $ ^ {-1}的模型重现。如果排放来自激风,则风速和$ 10 ^ {-7} $ M $ _ \ odot $ yr $ ^ {-1} $质量损失率。如果排放来自内部自由风区,则更快,更不密集的风将再现Br $ \γ$的光度。膨胀的彗星风泡在潮气通过后的几年里发生了变化,这主要是由于潮汐与黑洞的相互作用而被破坏了。

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