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NEAR-INFRARED DETECTION OF A SUPER-THIN DISK IN NGC?891

机译:NGC?891中超薄盘的近红外检测

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We probe the disk structure of the nearby, massive, edge-on spiral galaxy NGC?891 with subarcsecond resolution JHK s-band images covering ~ ±10?kpc in radius and ±5?kpc in height. We measure intrinsic surface brightness (SB) profiles using realistic attenuation corrections constrained from near- and mid-infrared (Spitzer) color maps and three-dimensional Monte Carlo radiative-transfer models. In addition to the well-known thin and thick disks, a super-thin disk with 60-80?pc scale-height—comparable to the star-forming disk of the Milky Way—is visibly evident and required to fit the attenuation-corrected light distribution. Asymmetries in the super-thin disk light profile are indicative of young, hot stars producing regions of excess luminosity and bluer (attenuation-corrected) near-infrared color. To fit the inner regions of NGC?891, these disks must be truncated within ~3?kpc, with almost all their luminosity redistributed in a bar-like structure 50% thicker than the thin disk. There appears to be no classical bulge but rather a nuclear continuation of the super-thin disk. The super-thin, thin, thick, and bar components contribute roughly 30%, 42%, 13%, and 15% (respectively) to the total K s-band luminosity. Disk axial ratios (length/height) decrease from 30 to 3 from super-thin to thick components. Both exponential and sech2 vertical SB profiles fit the data equally well. We find that the super-thin disk is significantly brighter in the K s-band than typically assumed in integrated spectral energy distribution models of NGC?891: it appears that in these models the excess flux, likely produced by young stars in the super-thin disk, has been mistakenly attributed to the thin disk.
机译:我们用亚秒分辨率的JHK s波段图像探测了附近巨大的边缘螺旋星系NGC?891的盘结构,该图像的半径约为±10?kpc,高度约为±5?kpc。我们使用受近红外和中红外(Spitzer)彩色图和三维蒙特卡洛辐射传递模型约束的现实衰减校正来测量固有表面亮度(SB)轮廓。除了众所周知的薄磁盘和厚磁盘,明显可见的标尺高度为60-80?pc的超薄磁盘(与银河系中形成恒星的磁盘相当),需要使用它来校正衰减配光。超薄圆盘光剖面中的不对称性表示年轻的炽热恒星产生了过多的光度和蓝色(经衰减校正)的近红外色区域。为了适合NGC?891的内部区域,这些磁盘必须在约3kkpc内被截断,几乎所有的光度都以棒状结构重新分布,其厚度比薄磁盘厚50%。似乎没有经典的凸起,而是超薄磁盘的核延续。超薄,薄,厚和条形成分分别占K s波段总亮度的大约30%,42%,13%和15%。磁盘轴向比(长/高)从30降低到3,从超薄组件变为厚组件。指数和sech2垂直SB配置文件均很好地拟合了数据。我们发现,在K s波段,超薄盘的亮度比NGC?891的综合光谱能量分布模型中通常假定的要亮得多:在这些模型中,似乎是由超新星产生的过剩通量精简磁盘,已被错误地归因于精简磁盘。

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