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No asymmetric outflows from Sagittarius A* during the pericenter passage of the gas cloud G2

机译:在气云G2的中心点通过期间没有来自人马座A *的不对称流出

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The gas cloud G2 that falls toward Sagittarius A* (Sgr A*), the supermassive black hole at the center of the Milky Way, is assumed to provide valuable information on the physics of accretion flows and the environment of the black hole. We observed Sgr A* with four European stations of the Global Millimeter Very Long Baseline Interferometry Array (GMVA) at 86 GHz on 1 October 2013 when parts of G2 had already passed the pericenter. We searched for a possible transient asymmetric structure – such as jets or winds from hot accretion flows – around Sgr A* that might be caused by accretion of material from G2. The interferometric closure phases remained zero within errors during the observation time. We therefore conclude that Sgr A* did not show significant asymmetric (in the observer frame) outflows in late 2013. Using simulations, we constrain the size of the outflows that we could have missed to ≈2.5 mas along the major axis and ≈0.4 mas along the minor axis of the beam, corresponding to approximately 232 and 35 Schwarzschild radii, respectively; we thus probe spatial scales on which the jets of radio galaxies are thought to convert magnetic into kinetic energy. Because probably less than 0.2 Jy of the flux from Sgr A* can be attributed to accretion from G2, the effective accretion rate is η? ? 1.5 × 109 kg s-1 ≈ 7.7 × 10-9M⊕ yr-1 for material from G2. Exploiting the relation of kinetic jet power to accretion power of radio galaxies shows that the rate of accretion of matter that is finally deposited in jets is limited to ? ? 1017 kg s-1 ≈ 0.5 M⊕ yr-1. Accordingly, G2 appears to be mostly stable against loss of angular momentum and subsequent (partial) accretion at least on timescales ?1 yr.
机译:朝着射手座A *(Sgr A *)(位于银河系中心的超大质量黑洞)掉落的气云G2被认为可提供有关吸积流物理学和黑洞环境的有价值的信息。我们在2013年10月1日观测到了Sgr A *在86 GHz处的全球毫米毫米极长基线干涉测量阵列(GMVA)的四个欧洲站点,当时G2的一部分已经通过了近心点。我们搜索了Sgr A *附近可能存在的瞬态非对称结构,例如喷射或来自热积聚流的风,这可能是由G2物质积聚引起的。在观察时间内,误差闭合阶段在误差范围内保持为零。因此,我们得出的结论是,Sgr A *在2013年末没有出现显着的非对称(在观察者框架内)流出。使用模拟,我们将沿主轴线可能错过的流出量限制为≈2.5 mas,而将错过的流出量限制为≈0.4 mas沿光束的短轴,分别对应于约232和35的Schwarzschild半径;因此,我们探究了被认为是射电星系射流将磁转换为动能的空间尺度。因为来自Sgr A *的磁通量可能少于0.2 Jy可归因于来自G2的积聚,所以有效积聚率为η?。 ?对于G2中的材料,为1.5×109千克s-1≈7.7×10-9M⊕yr-1。利用动射流功率与射电星系的积聚功率之间的关系,可以发现最终沉积在射流中的物质的积聚速率被限制为? ? 1017千克s-1≈0.5M⊕yr-1。因此,G2似乎在至少角速度≥1年的时间内对角动量的损失和随后的(部分)增生几乎是稳定的。

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