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Very Extended X-Ray and Hα Emission in M82: Implications for the Superwind Phenomenon

机译:M82中极广的X射线和Hα发射:对超风现象的影响

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We discuss the properties and implications of the recently discovered 35 × 09 (3.7 × 0.9 kpc) region of spatially coincident X-ray and Hα emission about 11' (11.6 kpc) to the north of the prototypical starburst/superwind galaxy M82. The total Hα flux from this ridge of emission is 1.5 × 10-13 ergs s-1 cm -2, or about 0.3% of the total M82 Hα flux. The implied Hα luminosity of this region is 2.4 × 1038 ergs s-1. Diffuse soft X-ray emission is seen over the same region by the ROSAT PSPC and HRI. The PSPC X-ray spectrum is fitted by thermal plasma absorbed by only the Galactic foreground column density (NH = 3.7 × 1020 cm-2) and having a temperature of kT = 0.80 ± 0.17 keV. The total unabsorbed flux from the ridge is 1.4 × 10-13 ergs cm-2 s-1 (~2.2 × 1038 ergs s-1), comprising about 0.7% of the total X-ray emission from M82. We evaluate the relationship of the X-ray/Hα ridge to the M82 superwind. The Hα emission could be excited by ionizing radiation from the starburst that propagates into the galactic halo along the cavity carved by the superwind. However, the main properties of the X-ray emission can all be explained as being due to shock heating driven as the superwind encounters a massive ionized cloud in the halo of M82 (possibly related to the tidal debris seen in H I in the interacting M81/M82/NGC 3077 system). This encounter drives a slow shock into the cloud, which contributes to the excitation of the observed Hα emission. At the same time, a fast bow shock develops in the superwind just upstream of the cloud, and this produces the observed X-ray emission. This interpretation would imply that the superwind has an outflow speed of roughly 800 km s-1, consistent with indirect estimates based on its general X-ray properties and the kinematics of the inner kiloparsec-scale region of Hα filaments. The alternative, in which a much faster and more tenuous wind drives a fast radiative shock into a cloud that then produces both the X-ray and Hα emission, is ruled out by the long radiative cooling times and the relatively quiescent Hα kinematics in this region. We suggest that wind-cloud interactions may be an important mechanism for generating X-ray and optical line emission in the halos of starbursts. Such interactions can establish that the wind has propagated out to substantially greater radii than could otherwise be surmised. This has potentially interesting implications for the fate of the outflowing metal-enriched material, and bears on the role of superwinds in the metal enrichment and heating of galactic halos and the intergalactic medium. In particular, the gas in the M82 ridge is roughly 2 orders of magnitude hotter than the minimum "escape temperature" at this radius, so this gas will not be retained by M82.
机译:我们讨论了在原型星爆/超风星系M82以北约11'(11.6 kpc)的空间发现的X射线和Hα发射的35×09(3.7×0.9 kpc)区域的性质和含义。来自该发射脊的总Hα通量为1.5×10-13 ergs s-1 cm -2,约占M82Hα总通量的0.3%。该区域的隐含Hα发光度为2.4×1038 ergs s-1。 ROSAT PSPC和HRI在同一区域看到了漫射软X射线发射。 PSPC X射线光谱由仅被Galactic前景柱密度(NH = 3.7×1020 cm-2)吸收且温度为kT = 0.80±0.17 keV的热等离子体拟合。来自脊的总未吸收通量为1.4×10-13 ergs cm-2 s-1(〜2.2×1038 ergs s-1),约占M82总X射线发射量的0.7%。我们评估了X射线/Hα脊与M82超风的关系。 Hα的发射可以通过电离星爆的辐射而激发,该辐射沿着超风雕刻的空腔传播到银河晕中。但是,X射线发射的主要特性都可以解释为是由于超风在M82的晕圈中遇到了巨大的电离云而驱动了激波加热(可能与HI在相互作用的M81 /中看到的潮汐碎片有关)。 M82 / NGC 3077系统)。这次相遇将缓慢的冲击带入云层,这有助于激发观察到的Hα发射。同时,在云的上游的超风中会产生快速的弓形冲击,这会产生观察到的X射线发射。这种解释将暗示,超风的流出速度约为800 km s-1,这与基于其一般X射线特性和Hα细丝内部千帕尺度区域的运动学得出的间接估计一致。替代方法是,较长的辐射冷却时间和该区域相对静止的Hα运动学原理排除了这种替代方法,即更快,更弱的风将快速的辐射冲击驱入云中,然后产生X射线和Hα辐射。 。我们建议,风云相互作用可能是在星爆光晕中产生X射线和光学线发射的重要机制。这样的相互作用可以确定风已经传播到比原本可以推测的大得多的半径。这对流出的富含金属的物质的命运具有潜在的有趣意义,并涉及超风在银晕和星际介质的金属富集和加热中的作用。特别是,M82脊中的气体比该半径处的最小“逸出温度”高大约2个数量级,因此该气体不会被M82保留。

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