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首页> 外文期刊>The Astrophysical journal >GALACTIC WIND IN THE NEARBY STARBURST GALAXY NGC 253 OBSERVED WITH THE KYOTO3DII FABRY-PEROT MODE
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GALACTIC WIND IN THE NEARBY STARBURST GALAXY NGC 253 OBSERVED WITH THE KYOTO3DII FABRY-PEROT MODE

机译:使用KYOTO3DII FABRY-PEROT模式观察到的附近星暴银河NGC 253中的银河风

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We have observed the central region of the nearby starburst galaxy NGC 253 with the Kyoto Tridimensional Spectrograph II Fabry-Perot mode in order to investigate the properties of its galactic wind. Since this galaxy has a large inclination, it is easy to observe its galactic wind. We produced the Hα, [N II]λ6583, and [S II]λλ6716,6731 images, as well as their line-ratio maps. The [N II]/Hα ratio in the galactic-wind region is larger than those in H II regions in the galactic disk. The [N II]/Hα ratio in the southeastern filament, a part of the galactic wind, is the largest and reaches about 1.5. These large [N II]/Hα ratios are explained by shock ionization/excitation. Using the [S II]/Hα ratio map, we spatially separate the galactic-wind region from the starburst region. The kinetic energy of the galactic wind can be sufficiently supplied by supernovae in a starburst region in the galactic center. The shape of the galactic wind and the line-ratio maps are nonaxisymmetric about the galactic minor axis, which is also seen in M82. In the [N II]λ6583/[S II]λλ6716,6731 map, the positions with large ratios coincide with the positions of star clusters found in the Hubble Space Telescope observation. This means that intense star formation causes strong nitrogen enrichment in these regions. Our unique data of the line-ratio maps including [S II] lines have demonstrated their effectiveness for clearly distinguishing between shocked-gas regions and starburst regions, determining the extent of galactic wind and its mass and kinetic energy, and discovering regions with enhanced nitrogen abundance.
机译:为了研究其银河风的性质,我们用《京都三维三维光谱图II》法布里-珀罗模式观察了附近爆炸星系NGC 253的中心区域。由于该星系的倾角很大,因此很容易观察到它的银河风。我们制作了Hα,[N II]λ6583和[S II]λλ6716,6731图像,以及它们的线比图。银河风区的[N II] /Hα比大于银河盘中H II区的[N II] /Hα比。东南长丝(银河风的一部分)中的[N II] /Hα比最大,约为1.5。这些大的[N II] /Hα比值可以通过电离/激发来解释。使用[S II] /Hα比图,我们在空间上将星系风区域与星爆区域分开。银河风的动能可以由超新星在银河中心的星爆区域中充分提供。银河风的形状和线比例图关于银短轴是非轴对称的,这在M82中也可以看到。在[N II]λ6583/ [S II]λλ6716,6731图中,比率较大的位置与在哈勃太空望远镜观测中发现的星团的位置重合。这意味着强烈的恒星形成会在这些区域引起强烈的氮富集。我们包含[S II]线的线比率图的独特数据证明了其在清楚地区分冲击气体区域和星暴区域,确定银河风的范围及其质量和动能以及发现氮含量提高的区域方面的有效性。丰富。

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