费米子场下修正量子引力中的暴胀

Sh.R. Myrzakulov, Y. Myrzakulov, R. Yechshanova, М. Imankul
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引用次数: 1

摘要

利用量子方法研究了修正非均匀各向同性F(R)引力在F -本质费米子场中的可行膨胀。它的作用是S=\int[],其中R是曲率标量,Lm是物质拉格朗日量。在这种情况下,我们考虑一个非最小耦合费米子场f-本质,它的拉格朗日量由K(Y,u)表示,它由一个依赖于Y-动力学参数和u -势参数的函数表示。得到了齐次各向同性弗里德曼-罗伯逊-沃克时空下该模型的运动方程。作为F(R),我们考虑广义Horava-Lifshitz量子引力函数。2009年,Horava提出了一种在量子引力理论中研究膜的新方法,称为Horava- lifshitz引力。Horava-Lifshitz引力的特点是它是可重整的。进一步研究了K(Y,u)=lnY+u的特殊情况。得到了描述当前宇宙加速膨胀的参数,确定了物质与时空联系的显式形式h(u)。研究了模型演化的暴胀期。为了描述暴胀期,确定了哈勃参数和慢滚降参数的形式,以及其他暴胀参数。所得结果与观测结果进行了比较。分析结果与解中某些积分常数值处的观测数据吻合。
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Inflation in modified quantum gravity with a fermion field
Viable inflation of modified nonuniform isotropic F(R) gravity with a fermionic field of f-essence is investigated using the quantum approach. The action of which is S=\int [], where R is the curvature scalar, and Lm is the matter Lagrangian. In this case, we consider a non-minimally coupled fermionic field f-essence, the Lagrangian of which is denoted by K(Y,u) by a function depending on Y-kinetic and u potential arguments. The equations of motion of this model are obtained for the homogeneous and isotropic Friedman-Robertson-Walker space-time. As F(R) we consider the generalized Horava-Lifshitz quantum gravity function. In 2009, Horava proposed a new approach to studying membranes in the theory of quantum gravity, known as the Horava-Lifshitz gravity.The peculiarity of Horava-Lifshitz gravity is that it is renormalizable. Further, the particular case of K(Y,u)=lnY+u is investigated in detail. The parameters of describing the current accelerated expansion of the Universe are obtained and the explicit form of the connection of matter with space-time h(u) is determined. The inflationary period of the evolution of this model is also investigated. To describe the inflationary period, the form of the Hubble parameter and the slow roll-off parameter, as well as other inflationary parameters, were determined. The presented results are compared with the observation results. The analysis of the results coincides with the observation data at certain values of the integral constants in the solutions.
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