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首页> 外文期刊>The Astrophysical journal >COSMIC MICROWAVE BACKGROUND ANISOTROPIES FROM THE REES-SCIAMA EFFECT IN Ω_0 ≤ 1 UNIVERSES
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COSMIC MICROWAVE BACKGROUND ANISOTROPIES FROM THE REES-SCIAMA EFFECT IN Ω_0 ≤ 1 UNIVERSES

机译:Ω_0≤1个宇宙中REES-SCIAMA效应引起的宇宙微波背景各向异性

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摘要

We investigate the imprint of nonlinear matter condensations on the cosmic microwave background (CMB) in Ω_0 < 1 cold dark matter (CDM) model universes with simulation domains ranging from 120 h~(-1) Mpc to 360 h~(-1) Mpc in size. We concentrate on the secondary temperature anisotropies induced by time varying gravitational potentials occurring after decoupling. Specifically, we investigate the importance of the Rees-Sciama effect due to: (1) intrinsic changes in the gravitational potential of forming, nonlinear structures; (2) proper motion of nonlinear structures; and (3) late-time decay of gravitational potential perturbations in open universes. CMB temperature anisotropies are obtained by numerically evolving matter inhomogeneities and CMB photons from an early, linear epoch (z = 100) to the present, nonlinear epoch (z = 0). We test the dependence and relative importance of these secondary temperature anisotropies as a function of the scale of the underlying matter (voids, superclusters) and as a function of Ω_0. The results of the Ω_0 < 1 models are compared to a similarly executed Ω_0 = 1 simulation. We find that in low-density models all three sources of anisotropy can be relevant, reaching levels of ΔT/T ~ 10~(-6). We also find that, for Ω_0 < 1, at large scales the secondary temperature anisotropies are dominated by the decaying potential.
机译:我们研究了Ω_0<1冷暗物质(CDM)模型宇宙中宇宙物质微波背景(CMB)上非线性物质凝聚的烙印,其模拟域范围为120 h〜(-1)Mpc至360 h〜(-1)Mpc在尺寸方面。我们专注于解耦后发生的时变重力势所引起的二次温度各向异性。具体来说,我们研究Rees-Sciama效应的重要性,这是由于:(1)形成的非线性结构的引力的内在变化; (2)非线性结构的适当运动; (3)开放宇宙中引力势扰动的后期衰减。 CMB温度各向异性是通过从早期线性时期(z = 100)到当前非线性时期(z = 0)数值演化物质不均匀性和CMB光子获得的。我们测试了这些次要温度各向异性的依存性和相对重要性,这些依赖关系和相对重要性是作为基础物质(空隙,超团簇)的尺度的函数,并且是Ω_0的函数。将Ω_0<1模型的结果与类似执行的Ω_0= 1仿真进行比较。我们发现,在低密度模型中,各向异性的所有三个来源都是相关的,达到ΔT/ T〜10〜(-6)的水平。我们还发现,对于Ω_0<1,在较大范围内,次级温度各向异性主要由衰减电位决定。

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