An approximate application of quantum gravity to the rotation problem

Richard Michael Jones
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Abstract

{Arbitrary initial conditions allow solutions of Einstein's field equations for General Relativity to have arbitrarily large relative rotation of matter and inertial frames. The ``Rotation Problem'' is to explain why the measured relative rotation rate is so small. As it turns out, nearly any reasonable theory of quantum gravity can solve the rotation problem by phase interference.} Even as early as {}{about a quarter of a second after the initial simgularity, quantum cosmology would limit the cosmologies that contribute significantly to a path integral calculation to have relative rms rotation rates less than about} {{}}{$10^{-51}$ radians per year.} Those calculations are based on using 50 e-foldings during inflation. For 55 or 60 e-foldings, the cosmologies contributing significantly to the path integral would have even smaller relative rotation rates. In addition, although inflation dominates the calculation, even if there had been no inflation, the cosmologies contributing significantly to the path integral would have relative rotation rates less than about {}{$10^{-32}$ radians per year at about a quarter of a second after the initial singularity.} These calculations are insensitive to the details of the theory of quantum gravity because the main factor depends only on the size of the visible universe, the Planck time, the free-space speed of light, the Hubble parameter, and the number of e-foldings during inflation. These calculations use the Einstein-Hilbert action in quantum gravity, {{}}{including} large-scale relative rotation of inertial frames and the matter distribution, in which each ``path'' is a cosmology with a different rms relative rotation rate. The calculations include inflation for 50, 55, and 60 e-foldings, and for values of the dependence of relative rotation rate on cosmological scale factor $a$ as $a^{-m}$ for various values of $m$. The calculation shows that the action is an extremum at zero rms relative rotation rate.
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量子引力在旋转问题上的近似应用
{任意的初始条件使得广义相对论爱因斯坦场方程的解具有任意大的物质和惯性框架的相对旋转。旋转问题 "旨在解释为什么测得的相对旋转率如此之小。事实证明,几乎所有合理的量子引力理论都能通过相位干涉解决旋转问题。}甚至早在{}{初始模拟后约四分之一秒,量子宇宙学就会限制对路径积分计算有重大贡献的宇宙学,使其相对均方根旋转率小于每年约}{}{$10^{-51}$弧度。这些计算是基于在膨胀过程中使用50个电子折叠。对于 55 或 60 个 e-foldings,对路径积分有重要贡献的宇宙将具有更小的相对旋转率。此外,虽然通货膨胀在计算中占主导地位,但即使没有通货膨胀,在初始奇点后约四分之一秒时,对路径积分有重要贡献的宇宙学的相对旋转率也会小于每年约{}{$10^{-32}$弧度。}这些计算对量子引力理论的细节并不敏感,因为主要因素只取决于可见宇宙的大小、普朗克时间、自由空间光速、哈勃参数以及膨胀过程中电子折叠的数量。这些计算使用了量子引力中的爱因斯坦-希尔伯特作用,{{}{包括}惯性框架的大尺度相对旋转和物质分布,其中每条 "路径 "都是具有不同均方根相对旋转率的宇宙学。计算包括50、55和60电子折叠的膨胀,以及相对旋转率对宇宙学尺度因子$a$的依赖值,即在不同的$m$值下的$a^{-m}$。计算结果表明,在均方根相对旋转率为零时,作用是一个极值。
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