首页> 外文期刊>The Astrophysical journal >KINEMATICS OF LOW-z ULTRALUMINOUS INFRARED GALAXIES AND IMPLICATIONS FOR DYNAMICAL MASS DERIVATIONS IN HIGH-z STAR-FORMING GALAXIES
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KINEMATICS OF LOW-z ULTRALUMINOUS INFRARED GALAXIES AND IMPLICATIONS FOR DYNAMICAL MASS DERIVATIONS IN HIGH-z STAR-FORMING GALAXIES

机译:低z红外超星系的运动学及其对高z星系星系动力学质量衍生的启示

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摘要

The kinematic properties of the gaseous and stellar components of 11 ultraluminous infrared galaxies (ULIRGs; 14 nuclei) are investigated by means of integral field spectroscopy (IFS) with the INTEGRAL system and available IR and CO millimeter spectroscopy. The sample of ULIRGs cover different phases of the merging process and span all levels of activity from pure starbursts to Seyfert nuclei. The IFS data show that the ionized gas has a complex velocity structure with peak-to-peak velocity differences of a few to several hundred km s~(-1), detected in tidal tails or extranuclear star-forming regions. The velocity field of the ionized gas on scales of a few to several kiloparsecs is dominated by tidally induced flows and does not, in general, correspond to rotationally supported systems with a privileged orientation along the major rotating axis. The central velocity amplitude of the ionized gas and stars shows discrepancies in some galaxies but has, on average, a similar value (ratio of 0.92 ± 0.37), while the velocity amplitude of the molecular gas is a factor of 2 larger (ratio of 1.9 ± 0.6) than that of the stars and ionized gas. The central velocity amplitude measured using different kinematic tracers should therefore not be used in ULIRGs as a reliable tracer of mass, in general. The IFS data also show that the velocity dispersion of the ionized gas maps the large-scale motions associated with tidal tails and extranuclear regions, with often the highest velocity dispersion not being associated with the nucleus galaxies. There is, however, a good agreement between the central ionized gas and stellar velocity dispersions (ratio of 1.01 ± 0.13), while the cold molecular gas velocity dispersion has lower values (average of about 0.8 that of the stellar and ionized gas). The central ionized gas velocity dispersion is therefore a robust and homogeneous observable and a good tracer of the dynamical mass in these systems. The IFS-based central ionized gas velocity dispersion measurements confirm that ULIRGs' hosts are moderate-mass (≤ m_*) galaxies, as previously concluded by Tacconi and coworkers. In general, velocity amplitudes should not be used to estimate the dynamical mass in high-z star-forming systems, such as Lyman break and in particular submillimeter galaxies, since they show irregular stellar and gaseous structures similar to those present in low-z merging systems such as ULIRGs, the subject of this study. A more reliable method is to measure the central velocity dispersion using the strong, high equivalent width, rest-frame optical emission lines, provided the location of the nucleus is independently established by high angular resolution red or near-IR rest-frame imaging. The kinematics derived from the millimeter CO line suggest that the cold gas in ULIRGs does not share the velocity field of the stars and ionized gas and seems to be more rotationally supported. This result needs to be investigated in more detail with a larger sample of low-z ULIRGs before using the millimeter CO line widths as a dynamical mass tracer in high-z submillimeter galaxies.
机译:通过具有INTEGRAL系统的积分光谱仪(IFS)以及可用的IR和CO毫米波光谱仪,研究了11个超发光红外星系(ULIRGs; 14原子核)的气态和恒星组分的运动学特性。 ULIRG样品涵盖了合并过程的不同阶段,涵盖了从纯星爆到塞弗特核的所有活动水平。 IFS数据表明,电离气体具有复杂的速度结构,在潮汐尾部或核外恒星形成区域中检测到的峰峰速度差为几公里至几百公里s〜(-1)。电离气体的速度场在几到几千帕斯卡的范围内,主要由潮汐流引起,通常不对应于沿主旋转轴优先定向的旋转支撑系统。电离气体和恒星的中心速度振幅在某些星系中显示出差异,但平均而言具有相似的值(比率0.92±0.37),而分子气体的速度振幅则大2倍(比率1.9) ±0.6)比恒星和电离气体要大。因此,通常不应将使用不同运动学示踪剂测得的中心速度幅度用作可靠的质量示踪剂在ULIRG中。 IFS数据还显示,电离气体的速度色散映射了与潮汐尾巴和核外区域相关的大规模运动,其中最高速度色散通常与核星系无关。但是,中心电离气体和恒星速度散度之间有很好的一致性(比率为1.01±0.13),而冷分子气体的速度散度具有较低的值(平均值约为恒星和电离气体的0.8)。因此,在这些系统中,中心电离气体速度弥散是可靠且均匀的可观测值,并且是动态质量的良好示踪剂。基于IFS的中央电离气体速度弥散度测量结果证实,ULIRG的宿主是中等质量(≤m_ *)星系,正如Tacconi及其同事先前得出的结论。通常,不应使用速度振幅来估算高z星形成系统(例如莱曼破裂,尤其是亚毫米星系)中的动态质量,因为它们显示出与低z合并中相似的不规则恒星和气态结构ULIRG等系统,是本研究的主题。一种更可靠的方法是使用强的,高等效宽度的静止帧光发射线来测量中心速度色散,前提是通过高角度分辨率红色或近红外静止帧成像独立地确定原子核的位置。从毫米CO线得出的运动学表明,ULIRG中的冷气体与恒星和离子化气体没有速度场,并且似乎受到更多的旋转支撑。在使用毫米CO线宽作为高z亚毫米星系中的动态质量示踪剂之前,需要使用较大的低z ULIRG样本来更详细地研究此结果。

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