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首页> 外文期刊>The Astrophysical journal >CHANDRA OBSERVATIONS OF EXPANDING SHELLS IN THE DWARF STARBURST GALAXY NGC 3077
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CHANDRA OBSERVATIONS OF EXPANDING SHELLS IN THE DWARF STARBURST GALAXY NGC 3077

机译:矮星型星系NGC 3077膨胀壳的CHANDRA观测

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摘要

Deep Chandra observations (53 ks, ACIS-S3) of NGC 3077, a starburst dwarf galaxy in the M81 triplet, resolve the X-ray emission from several supershells. The emission is brightest in the cavities defined by expanding shells detected previously in Hα emission. Thermal emission models fitted to the data imply temperatures ranging from ~1.3 to 4.9 x 10~6 K and indicate that the strongest absorption is coincident with the densest clouds traced by CO emission. The fitted emission measures give pressures of P/k ≈ (10~5-10~6)ξ~(-0.5)f_v~(-0.5) K cm~(-3) (where ξ is the metallicity of the hot gas in solar units and f_v is the volume filling factor). Despite these high pressures, the radial density profile of the hot gas is not as steep as that expected in a freely expanding wind (e.g., as seen in the neighboring starburst galaxy M82), implying that the hot gas is still confined by the Hα shells. The chaotic dynamical state of NGC 3077 undermines reliable estimates of the escape velocity. The more relevant quantity for the ultimate fate of the outflow is probably the gas density in the rich intragroup medium. Based on the H I distribution of NGC 3077 and a connected tidal tail we argue that the wind has the potential to leave the gravitational well of NGC 3077 to the north but not to the south. The total 0.3-6.0 keV X-ray luminosity is ~(2-5) x 10~(39) ergs s~(-1) (depending on the selected thermal plasma model). Most (~85%) of the X-ray luminosity in NGC 3077 comes from the hot interstellar gas; the remainder comes from six X-ray point sources. In spite of previous claims to the contrary, we do not find X-ray emission originating from the prominent tidal tail near NGC 3077.
机译:NGC 3077的深Chandra观测结果(53 ks,ACIS-S3)是M81三重态中的星暴矮星系,它分解了几个超壳的X射线发射。在由先前在Hα发射中检测到的膨胀壳所定义的空腔中,发射最亮。根据数据拟合的热辐射模型表明温度范围为〜1.3至4.9 x 10〜6 K,并表明最强的吸收与CO排放所追踪的最密集的云一致。拟合的排放措施给出的压力为P / k≈(10〜5-10〜6)ξ〜(-0.5)f_v〜(-0.5)K cm〜(-3)(其中ξ是太阳能单位,f_v是体积填充因子)。尽管有这些高压,但热气的径向密度分布并不像自由扩展风中所预期的那样陡峭(例如,如在相邻的星爆星系M82中所见),这意味着热气仍受Hα壳层限制。 NGC 3077的混沌动力学状态破坏了逃逸速度的可靠估计。对于最终的流出命运而言,更相关的数量可能是富集团内部培养基中的气体密度。基于NGC 3077的H I分布和潮汐尾巴,我们认为风有可能使NGC 3077的重力井向北离开而不向南离开。 0.3-6.0 keV X射线的总发光度约为(2-5)x 10〜(39)ers s〜(-1)(取决于所选的热等离子体模型)。 NGC 3077中大部分(〜85%)的X射线发光度来自星际气体。其余的来自六个X射线源。尽管先前有相反的说法,但我们并未发现源自NGC 3077附近显着的潮汐尾的X射线发射。

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