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Classical and quantum Bianchi type III vacuum Ho?ava-Lifshitz cosmology

机译:经典和量子Bianchi III型真空Ho?ava-Lifshitz宇宙学

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A diagonal Bianchi type III spacetime is treated, both at the classical and quantum level, in the context of Ho?ava-Lifshitz gravity. The system of the classical equations of motion is reduced to one independent Abel's equation of the first kind. Closed form solutions are presented for various values of the coupling constants appearing in the action. Due to the method used, solutions of Euclidean, Lorentzian and neutral signatures are attained. The main general solution for λ = 1 is seen to contain a curvature singularity at t = 0, while in its Einsteinian limit it reproduces the known diagonal solution (with and/or without cosmological constant). The rest of the solutions correspond to somewhat isolated cases, as they emerge from either setting the coefficient of the lapse to zero or taking λ = 1/3. They are singularity free, but they all have a singular limit as the other constants approach their Einsteinian values. At the quantum level, the resulting Wheeler-DeWitt equation is explicitly solved for λ = 1, σ = 0 and λ = 1/3. The ensuing wave functions diverge in the Einsteinian limit.
机译:在Ho?ava-Lifshitz引力的背景下,对角线的Bianchi III型时空在古典和量子水平上都得到了处理。经典运动方程组简化为一个独立的第一类Abel方程。针对动作中出现的各种耦合常数值,提供了封闭形式的解决方案。由于使用了该方法,因此获得了欧几里得,洛伦兹和中性签名的解决方案。可以看到λ= 1的主要一般解在t = 0处包含曲率奇点,而在其爱因斯坦极限中,它重现了已知的对角线解(有和/或没有宇宙学常数)。其余解对应于有些孤立的情况,因为它们要么是将延迟系数设置为零,要么是λ= 1/3。它们没有奇点,但是当其他常数接近其爱因斯坦值时,它们都具有奇极限。在量子水平上,对于λ= 1,σ= 0和λ= 1/3明确求解Wheeler-DeWitt方程。随后的波函数在爱因斯坦极限中发散。

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