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Dark energy and extended dark matter halos

机译:暗能量和扩展暗物质光环

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The cosmological mean matter (dark and baryonic) density measured in the units of the critical density is Ωm?=?0.27. Independently, the local mean density is estimated to be Ωloc?=?0.08?0.23 from recent data on galaxy groups at redshifts up to z?=?0.01?0.03 (as published by Crook et?al. 2007, ApJ, 655, 790 and Makarov & Karachentsev 2011, MNRAS, 412, 2498). If the lower values of Ωloc are reliable, as Makarov & Karachentsev and some other observers prefer, does this mean that the Local Universe of 100–300?Mpc across is an underdensity in the cosmic matter distribution? Or could it nevertheless be representative of the mean cosmic density or even be an overdensity due to the Local Supercluster therein. We focus on dark matter halos of groups of galaxies and check how much dark mass the invisible outer layers of the halos are able to host. The outer layers are usually devoid of bright galaxies and cannot be seen at large distances. The key factor which bounds the size of an isolated halo is the local antigravity produced by the omnipresent background of dark energy. A gravitationally bound halo does not extend beyond the zero-gravity surface where the gravity of matter and the antigravity of dark energy balance, thus defining a natural upper size of a system. We use our theory of local dynamical effects of dark energy to estimate the maximal sizes and masses of the extended dark halos. Using data from three recent catalogs of galaxy groups, we show that the calculated mass bounds conform with the assumption that a significant amount of dark matter is located in the invisible outer parts of the extended halos, sufficient to fill the gap between the observed and expected local matter density. Nearby groups of galaxies and the Virgo cluster have dark halos which seem to extend up to their zero-gravity surfaces. If the extended halo is a common feature of gravitationally bound systems on scales of galaxy groups and clusters, the Local Universe could be typical or even an overdense region, with a low density contrast ?~1.
机译:以临界密度为单位测量的宇宙学平均物质(深色和重子)密度为Ωm?=?0.27。独立地,根据最近在红移直到z≥0.01≤0.03的星系组的数据,局部平均密度估计为Ωloc≥0.08≤0.23(如Crook et al。2007,ApJ,655,790所公布)。和Makarov&Karachentsev 2011,MNRAS,412,2498)。如果像Makarov&Karachentsev和其他一些观察家所喜欢的那样,较低的Ωloc值是可靠的,这是否意味着100-300?Mpc的局部宇宙在宇宙物质分布中是低密度的?但是它还是可以代表平均宇宙密度,甚至可以由于其中的局部超集群而成为超密度。我们关注星系群的暗物质晕,并检查晕的不可见外层能够容纳多少暗物质。外层通常没有明亮的星系,并且无法在远距离看到。限制孤立的光环大小的关键因素是无所不在的暗能量背景产生的局部反重力。引力束缚的光晕不会延伸到物质重力和暗能量反重力平衡的零重力表面,因此定义了系统的自然上限。我们使用暗能量局部动力学效应理论来估计扩展暗晕的最大尺寸和质量。使用来自三个最新星系组目录的数据,我们表明,计算出的质量边界符合以下假设:大量暗物质位于扩展光环的不可见外部,足以填补观测到的和预期的之间的间隙局部物质密度。附近的星系群和处女座星团都有暗晕,它们似乎一直延伸到零重力表面。如果扩展的光晕是万有引力约束系统在银河系群和星团尺度上的共同特征,那么局部宇宙可能是典型的甚至是一个超密度区域,密度对比值低至〜1。

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