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arXiv 1404.7825gr-qcastro-ph.COhep-th
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最小长度、弗里德曼方程和最大密度

Minimal Length, Friedmann Equations and Maximum Density

Adel Awad, Ahmed Farag Ali

摘要:

受Jacobson的热力学方法[gr-qc/9504004]的启发,Cai等人[hep-th/0501055,hep-th/0609128]已经证明了从热力学热力学第一定律中出现弗里德曼方程。我们扩展Akbar-Cai推导[hep-th/0609128]弗里德曼方程,以适应一般的熵面积定律。由广义不确定原理(GUP)推导出的熵-面积定律揭示了最大能量密度接近普朗克密度的存在性.允许一般连续压力$p(ρ,a)$导致有界曲率不变量和一般的非奇异演化。在这种情况下,最大能量密度是在有限的时间内达到的,并且在这一点之外没有宇宙学演化,这使得从时空的角度来看大爆炸奇点是不可接近的。最大能量密度和一般非奇异演化的存在性与状态方程和空间曲率$k$无关。作为一个例子,我们研究了状态方程$p=ωρ$的演化,通过它的相空间图来显示在有限时间内可达到的最大能量的存在。

英文摘要:

Inspired by Jacobson's thermodynamic approach[gr-qc/9504004], Cai et al [hep-th/0501055,hep-th/0609128] have shown the emergence of Friedmann equations from the first law of thermodynamics. We extend Akbar--Cai derivation [hep-th/0609128] of Friedmann equations to accommodate a general entropy-area law. Studying the resulted Friedmann equations using a specific entropy-area law, which is motivated by the generalized uncertainty principle (GUP), reveals the existence of a maximum energy density closed to Planck density. Allowing for a general continuous pressure $p(ρ,a)$ leads to bounded curvature invariants and a general nonsingular evolution. In this case, the maximum energy density is reached in a finite time and there is no cosmological evolution beyond this point which leaves the big bang singularity inaccessible from a spacetime prospective. The existence of maximum energy density and a general nonsingular evolution is independent of the equation of state and the spacial curvature $k$. As an example we study the evolution of the equation of state $p=ωρ$ through its phase-space diagram to show the existence of a maximum energy which is reachable in a finite time.

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