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1+3 covariant cosmic microwave background anisotropies II: The almost-Friedmann-Lemaitre model

机译:1 + 3协变宇宙微波背景各向异性II:几乎Friedman-Lemaitre模型

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lThis is the second of a series of papers extending the 1 + 3 covariant and gauge-invariant treatment of kinetic theory to an examination of cosmic microwave background temperature anisotropies arising from inhomogeneities in the early universe. The first paper (Paper Ij dealt with algebraic issues, representing anisotropies in a covariant and gauge-invariant way by means of projected symmetric and trace-free tensors. Here we derive the mode form of the integrated Boltzmann equations, first, giving a covariant version of the standard derivation using the mode recursion relations, second, demonstrating the link to the the multipole divergence equations and finally various analytic ways of solving the resulting equations are discussed. A general integral Form of solution is obtained for the equations with Thomson scattering. The covariant Friedmann-Lemaitre multipole form of the transport equations are found near tight-coupling using the covariant and gauge-invariant generalization of the Peebles and Yu expansion in Thompson scattering time. The dispersion relations and damping scale are then obtained from the covariant approach. The equations are integrated to give the covariant and gauge-invariant equivalent of the canonical scalar sourced anisotropies in the K = 0 (flat background) case. We carry out a simple treatment of the matter dominated free-streaming projection, slow-decoupling, and tight-coupling cases in covariant and gauge-invariant theory, with the aim of both giving a unified transparent derivation of this range of results and clarifying the formal connection between the usual approaches (for example, works by Hu and Sugiyama) and the covariant and gauge-invariant like treatments for scalar perturbations (for example, works by Challinor and Lasenby). (C) 2000 Academic Press. [References: 86]
机译:l这是将动力学理论的1 + 3协变和规范不变处理扩展到检查由早期宇宙中的不均匀性引起的宇宙微波背景温度各向异性的系列论文中的第二篇。第一篇论文(纸Ij涉及代数问题,通过投影对称和无迹线张量以协变和规范不变的方式表示各向异性。在这里,我们推导积分Boltzmann方程的模态形式,首先,给出协变形式使用模态递归关系进行标准推导的方法,其次,说明与多极散度方程的联系,最后讨论了各种求解结果方程的解析方法,并获得了带有汤姆森散射的方程的一般积分解。利用Peebles的协变量和规范不变的泛化以及汤普森散射时间的Yu展开,在紧耦合附近找到了输运方程的协变Friedmann-Lemaitre多极形式,然后从协变方法中获得了色散关系和阻尼尺度。方程被积分以给出正则s的协变和规范不变等价形式在K = 0(平坦背景)的情况下来自标量的各向异性。我们对协变和规范不变理论中的以物质为主的自由流动投影,慢速解耦和紧耦合情况进行了简单的处理,目的是对结果范围进行统一透明的推导,并阐明常规方法(例如Hu和Sugiyama的作品)与标量摄动的协变和规范不变式处理(例如Challinor和Lasenby的作品)之间的形式联系。 (C)2000年学术出版社。 [参考:86]

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