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arXiv 1707.03439astro-ph.COgr-qchep-phhep-th
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封闭宇宙中的暴胀

Inflation in a closed universe

Bharat Ratra

摘要:

为了得到封闭宇宙中能量密度不均匀性的功率谱,我们研究了一个空间封闭的暴胀修正的热大爆炸模型,该模型的演化历史分为三个时期:早期的缓慢滚动的标量场暴胀时期和通常的辐射和非相对论物质时期. (For我们的目的是没有必要考虑一个最终的暗能量占主导地位的时代。我们在每个历元中导出了相对论性线性微扰方程的通解。在膨胀时期的解决方案的积分常数确定从de Sitter不变的量子力学的初始条件的洛伦兹截面的膨胀封闭de Sitter空间来自霍金的处方,宇宙的量子态只包括场配置是正常的欧几里德(de Sitter)球截面。积分的辐射和物质的时代解决方案的常数是确定从加入的条件,通过要求线性微扰方程保持非奇异的时代之间的过渡。规范不变能量密度不均匀性的物质历元功率谱不是幂律,并且以期望推广到标准平坦空间标度不变功率谱的闭合模型的方式依赖于空间波数。我们得出的功率谱似乎不同于其他一些封闭的通货膨胀模型的功率谱,假设不同的(大概非德西特不变)初始条件。

英文摘要:

To derive a power spectrum for energy density inhomogeneities in a closed universe, we study a spatially-closed inflation-modified hot big bang model whose evolutionary history is divided into three epochs: an early slowly-rolling scalar field inflation epoch and the usual radiation and non-relativistic matter epochs. (For our purposes it is not necessary to consider a final dark energy dominated epoch.) We derive general solutions of the relativistic linear perturbation equations in each epoch. The constants of integration in the inflation epoch solutions are determined from de Sitter invariant quantum-mechanical initial conditions in the Lorentzian section of the inflating closed de Sitter space derived from Hawking's prescription that the quantum state of the universe only include field configurations that are regular on the Euclidean (de Sitter) sphere section. The constants of integration in the radiation and matter epoch solutions are determined from joining conditions derived by requiring that the linear perturbation equations remain nonsingular at the transitions between epochs. The matter epoch power spectrum of gauge-invariant energy density inhomogeneities is not a power law, and depends on spatial wavenumber in the way expected for a generalization to the closed model of the standard flat-space scale-invariant power spectrum. The power spectrum we derive appears to differ from a number of other closed inflation model power spectra derived assuming different (presumably non de Sitter invariant) initial conditions.

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