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arXiv 1903.04845gr-qcastro-ph.COhep-th
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模拟SU中的宇宙学(2)规范理论

Cosmology in Mimetic SU(2) Gauge Theory

Mohammad Ali Gorji, Shinji Mukohyama, Hassan Firouzjahi

摘要:

众所周知,标准标量场模拟宇宙学提供了类似暗物质的能量密度分量。在考虑$SU(2)$规范对称性的情况下,我们研究了空间平坦和弯曲FLRW时空中的模拟情形的规范场延拓。由于模拟约束,标准Yang-Mills项扮演宇宙学常数的角色,而模拟项提供两种不同的贡献:一种是标准辐射标度,如$ a^{-4}$;另一种是能量密度标度,如$\propto a^{-2}$。因此,在Friedmann方程中,我们有两种不同的能量密度,它们的尺度为$\propto a^{-2}$:一种是模拟的空间曲率,另一种是标准的空间曲率,它们可以相互竞争。在这种情况下,这两个贡献之间的简并被解开,因为模拟的空间曲率类项只出现在动力学水平,而标准的空间曲率项出现在动力学和运动学水平。

英文摘要:

It is well known that the standard scalar field mimetic cosmology provides a dark matter-like energy density component. Considering $SU(2)$ gauge symmetry, we study the gauge field extension of the mimetic scenario in spatially flat and curved FLRW spacetimes. Because of the mimetic constraint, the standard Yang-Mills term plays the role of the cosmological constant while the mimetic term provides two different contributions: one is the standard radiation scaling like $ a^{-4}$ while the other contribution in energy density scales as $\propto a^{-2}$. Consequently, in the Friedmann equation we have two different energy densities which scale as $\propto a^{-2}$: one is the mimetic spatial curvature-like and the other is the standard spatial curvature which can compete with each other. The degeneracy between these two contributions are disentangled in this scenario since the mimetic spatial curvature-like term shows up only at the dynamical level while the standard spatial curvature term shows up at both dynamical and kinematical levels.

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