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首页> 外文期刊>International journal of modern physics, D. Gravitation, astrophysics, cosmology >COSMOLOGICAL DYNAMICS OF f(R) GRAVITY SCALAR DEGREE OF FREEDOM IN EINSTEIN FRAME
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COSMOLOGICAL DYNAMICS OF f(R) GRAVITY SCALAR DEGREE OF FREEDOM IN EINSTEIN FRAME

机译:爱因斯坦框架中f(R)重力标度自由度的宇宙动力学

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f(R) gravity models belong to an important class of modified gravity models where the late time cosmic accelerated expansion is considered as a manifestation of the large scale modification of the force of gravity. f(R) gravity models can be expressed in terms of a scalar degree of freedom by redefinition of model's variable. The conformal transformation of the action from Jordan frame to Einstein frame makes the scalar degree of freedom more explicit and can be studied conveniently. We have investigated the features of the scalar degree of freedoms and the consequent cosmological implications of the power-law (ξR~n) and the Starobinsky (disappearing cosmological constant) f(R) gravity models numerically in the Einstein frame. Both the models show interesting behavior of their scalar degree of freedom and could produce the accelerated expansion of the universe in the Einstein frame with the negative equation of state of the scalar field. However, the scalar field potential for the power-law model is the well-behaved function of the field, whereas the potential becomes flat for higher value of field in the case of the Starobinsky model. Moreover, the equation of state of the scalar field for the power-law model is always negative and less than -1/3, which corresponds to the behavior of the dark energy, that produces the accelerated expansion of the universe. This is not always the case for the Starobinsky model. At late times, the Starobinsky model behaves as cosmological constant A as behaves by power-law model for the values of n → 2 at all times.
机译:f(R)重力模型属于一类重要的修改后的重力模型,其中晚宇宙加速膨胀被认为是重力大幅度修改的体现。 f(R)重力模型可以通过重新定义模型变量以标量自由度表示。从乔丹构架到爱因斯坦构架的共形变换使标量自由度更加明确,可以方便地进行研究。我们在爱因斯坦框架中以数字方式研究了标量自由度的特征以及幂律(ξR〜n)和Starobinsky(消失的宇宙学常数)f(R)引力模型的宇宙学含义。这两个模型都显示出标量自由度的有趣行为,并且可以在标量场状态为负的情况下在爱因斯坦框架中产生宇宙的加速膨胀。但是,幂律模型的标量场电势是场的良好功能,而对于Starobinsky模型,对于更高的场值,电势变得平坦。此外,幂律模型的标量场的状态方程始终为负且小于-1/3,这对应于暗能量的行为,产生了加速的宇宙膨胀。 Starobinsky模型并非总是如此。在后期,Starobinsky模型的行为一直像宇宙常数A一样,对于幂函数模型,n→2的值始终都像幂律模型一样。

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