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arXiv 1601.00547gr-qcastro-ph.COmath-phmath.MP
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关于宇宙学中的Hojman守恒量

On the Hojman conservation quantities in Cosmology

A. Paliathanasis, P. G. L. Leach, S. Capozziello

摘要:

我们讨论的应用Hojman的对称性方法的宇宙学守恒律的确定,这已被应用于不同的宇宙模型的不同作者最近。我们表明,Hojman的方法,经常哈密顿系统,其中的哈密顿函数是所涉及的系统的方程之一,是等价的应用Noether定理的广义变换。这意味着对于最小耦合标量场宇宙学或其他与标量场宇宙学共形相关的修正理论,如$f(R)$引力,Hojman方法的应用为我们提供了与Noether定理相同的结果。此外,我们还研究了特殊的Anonymous。$ϕ\left( t\right) =ϕ\left( a\left( t\right) \right) $,它已被引入到一个最小耦合标量场,我们研究了约化方程的Lie和Noether点对称性。我们表明,在这个Anterior下,该模型的未知函数不能被约束的要求存在的守恒定律和Hojman守恒量所产生的约化方程只不过是诺特守恒律的功能形式的自由粒子。另一方面,对于$f(T)$遥平行引力,不是Hojman守恒律的存在为我们提供了$f(T)$函数的特殊函数形式,而是要求约化的二阶微分方程允许Jacobi Last乘子,而新的守恒定律就是约化方程的Hamilton函数.

英文摘要:

We discuss the application of the Hojman's Symmetry Approach for the determination of conservation laws in Cosmology, which has been recently applied by various authors in different cosmological models. We show that Hojman's method for regular Hamiltonian systems, where the Hamiltonian function is one of the involved equations of the system, is equivalent to the application of Noether's Theorem for generalized transformations. That means that for minimally-coupled scalar field cosmology or other modified theories which are conformally related with scalar-field cosmology, like $f(R)$ gravity, the application of Hojman's method provide us with the same results with that of Noether's theorem. Moreover we study the special Ansatz. $ϕ\left( t\right) =ϕ\left( a\left( t\right) \right) $, which has been introduced for a minimally-coupled scalar field, and we study the Lie and Noether point symmetries for the reduced equation. We show that under this Ansatz, the unknown function of the model cannot be constrained by the requirement of the existence of a conservation law and that the Hojman conservation quantity which arises for the reduced equation is nothing more than the functional form of Noetherian conservation laws for the free particle. On the other hand, for $f(T)$ teleparallel gravity, it is not the existence of Hojman's conservation laws which provide us with the special function form of $f(T)$ functions, but the requirement that the reduced second-order differential equation admits a Jacobi Last multiplier, while the new conservation law is nothing else that the Hamiltonian function of the reduced equation.

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