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THE IMPACT OF THE GAS DISTRIBUTION ON THE DETERMINATION OF DYNAMICAL MASSES OF GALAXIES USING UNRESOLVED OBSERVATIONS

机译:气体分布对未解析观测值确定星系动态质量的影响

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Dynamical mass (M dyn) is a key property of any galaxy, yet a determination of M dyn is not straightforward if spatially resolved measurements are not available. This situation occurs in single-dish H I observations of the local universe, but also frequently in high-redshift observations. M dyn measurements in high-redshift galaxies are commonly obtained through observations of the CO line, the most abundant tracer of the molecular medium. Even though in most cases the CO line width can be determined with reasonable accuracy, a measurement of the size of the emitting region is typically challenging given current facilities. We show how the integrated spectra ("global profiles") of a variety of galaxy models depend on the spatial distribution of the tracer gas as well as its velocity dispersion. We demonstrate that the choice of tracer emission line (e.g., H I tracing extended, "flat," emission versus CO tracing more compact, "exponential," emission) significantly affects the shape of the global profiles. In particular, in the case of high (~50?km?s–1) velocity dispersions, compact tracers (such as CO) result in Gaussian-like (non-double-horned) profiles, as is indeed frequently seen in high-redshift observations. This leads to significantly different determinations of M dyn if different distributions of the tracer material ("flat" versus "exponential") are considered. We determine at which radii the rotation curve reaches the rotation velocity corresponding to the velocity width, and find that for each tracer this happens at a well-defined radius: H I velocity widths typically originate at ~5 optical scale lengths, while CO velocity widths trace the rotation velocity at ~2 scale lengths. We additionally explore other distributions to take into account that CO distributions at high redshift likely differ from those at low redshift. Our models, while not trying to reproduce individual galaxies, define characteristic radii that can be used in conjunction with the measured velocity widths in order to define dynamical masses consistent with the assumed gas distribution.
机译:动态质量(M dyn)是任何星系的关键属性,但是如果没有空间分辨的测量结果,则M dyn的确定并不简单。这种情况发生在局部宇宙的单碟H I观测中,但也经常发生在高红移观测中。高红移星系中的M dyn测量通常是通过观察CO线获得的,CO线是分子介质中最丰富的示踪剂。即使在大多数情况下,可以以合理的精度确定CO线宽,但是在给定当前设备的情况下,发射区尺寸的测量通常仍具有挑战性。我们展示了各种星系模型的积分光谱(“全局剖面”)如何取决于示踪气体的空间分布及其速度扩散。我们证明了示踪剂发射谱线的选择(例如,H示踪扩展,“平坦”排放与CO示踪更紧凑,“指数”排放)的选择会显着影响整体轮廓的形状。特别是在高速度色散(〜50?km?s-1)的情况下,紧凑的示踪剂(例如CO)会产生类似高斯(非双角)的轮廓,这在高光谱条件下确实经常出现红移观测。如果考虑到示踪剂材料的不同分布(“平坦”与“指数”),这将导致M dyn的显着不同。我们确定旋转曲线在哪个半径处达到与速度宽度相对应的旋转速度,并发现对于每个示踪剂,这都发生在明确定义的半径上:HI速度宽度通常起源于〜5光学刻度长度,而CO速度宽度追踪〜2标度长度的旋转速度。我们还探讨了其他分布,以考虑到高红移下的CO分布可能与低红移下的CO分布不同。我们的模型虽然未尝试复制单个星系,但定义了可与测得的速度宽度结合使用的特征半径,以定义与假定气体分布一致的动态质量。

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