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arXiv 1111.4474hep-th
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CFT驱动的量子宇宙学中的单值性和泛函行列式

Monodromies and functional determinants in the CFT driven quantum cosmology

A. O. Barvinsky, D. V. Nesterov

摘要:

本文应用单值方法计算一类特殊的二阶微分算子$F=-d^2/dτ^2+{\ddot g}/g$,$\ddot g= d^2g/dτ^2$的泛函行列式,该算子在周期边界条件下具有周期零模$g=g(τ)$ .这个算子出现在早期宇宙理论的应用中,特别是确定了由共形场论(CFT)产生的宇宙学中微正则系综的单圈统计和。这个系综通过将宇宙的无边界波函数的概念推广到一个特殊的准热态的水平来实现宇宙学初始条件的概念,该准热态由瞬子占主导地位,其振荡标度因子为欧几里得弗里德曼-罗伯逊-沃克度规。这些振荡导致了$F$的零模$g(τ)$的多节点性质,这是由Faddeev-Popov规范固定过程的方法从其约化的泛函行列式中测量出来的。计算是在欧几里得时间$τ$的周期范围内的多个节点(根)的一般情况下进行的,从而推广了以前已知的宇宙尺度因子的一个振荡的单节点情况下的结果。$F$的泛函行列式用其基函数的单值性表示,该基函数是在周期范围内连接相邻零模根对的时间段的贡献之和的求积式.

英文摘要:

We apply the monodromy method for the calculation of the functional determinant of a special second order differential operator $F=-d^2/dτ^2+{\ddot g}/g$, $\ddot g= d^2g/dτ^2$, subject to periodic boundary conditions with a periodic zero mode $g=g(τ)$. This operator arises in applications of the early Universe theory and, in particular, determines the one-loop statistical sum for the microcanonical ensemble in cosmology generated by a conformal field theory (CFT). This ensemble realizes the concept of cosmological initial conditions by generalizing the notion of the no-boundary wavefunction of the Universe to the level of a special quasi-thermal state which is dominated by instantons with an oscillating scale factor of their Euclidean Friedmann-Robertson-Walker metric. These oscillations result in the multi-node nature of the zero mode $g(τ)$ of $F$, which is gauged out from its reduced functional determinant by the method of the Faddeev-Popov gauge fixing procedure. The calculation is done for a general case of multiple nodes (roots) within the period range of the Euclidean time $τ$, thus generalizing the previously known result for the single-node case of one oscillation of the cosmological scale factor. The functional determinant of $F$ expresses in terms of the monodromy of its basis function, which is obtained in quadratures as a sum of contributions of time segments connecting neighboring pairs of the zero mode roots within the period range.

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