论文标题
Palatini $ f(\ Mathcal {r})$重力的可穿越薄壳虫洞的结构和稳定性
Structure and stability of traversable thin-shell wormholes in Palatini $f(\mathcal{R})$ gravity
论文作者
论文摘要
我们研究了在Palatini $ f(\ Mathcal {r})$ GRAVITY的背景下,以(球形对称)薄壳形成的可穿越的虫洞的结构和稳定性。我们发现,使用合适的结式形式主义,我们发现外壳上有效的自由度数量减少到一个单一的自由度,这将状态方程式固定为无质量的压力 - 能量领域的方程,这与一般的相对论性和度量$ f(r)$相反。另一个主要区别是,为了维持虫洞,所需的薄壳的表面能密度螺纹可以根据相应溶液的所需特征,甚至可能消失,甚至可能消失。我们通过通过手术嫁接Schwarzschild空间时间来构建薄壳虫洞来说明我们的结果,并证明这些配置始终是线性不稳定的。 However, surgically joined Reissner-Nordström space-times allow for linearly stable, traversable thin-shell wormholes supported by a positive energy density provided that the (squared) mass-to-charge ratio, given by $y=Q^2/M^2$, satisfies the constraint $1<y<9/8$ (corresponding to overcharged Reissner-Nordström configurations having a photon sphere) and lies in a region由特定曲线限制在壳的(无量纲)半径$ x_0 = r/m $的范围内。
We study the structure and stability of traversable wormholes built as (spherically symmetric) thin shells in the context of Palatini $f(\mathcal{R})$ gravity. Using a suitable junction formalism for these theories we find that the effective number of degrees of freedom on the shell is reduced to a single one, which fixes the equation of state to be that of massless stress-energy fields, contrary to the general relativistic and metric $f(R)$ cases. Another major difference is that the surface energy density threading the thin-shell, needed in order to sustain the wormhole, can take any sign, and may even vanish, depending on the desired features of the corresponding solutions. We illustrate our results by constructing thin-shell wormholes by surgically grafting Schwarzschild space-times, and show that these configurations are always linearly unstable. However, surgically joined Reissner-Nordström space-times allow for linearly stable, traversable thin-shell wormholes supported by a positive energy density provided that the (squared) mass-to-charge ratio, given by $y=Q^2/M^2$, satisfies the constraint $1<y<9/8$ (corresponding to overcharged Reissner-Nordström configurations having a photon sphere) and lies in a region bounded by specific curves defined in terms of the (dimensionless) radius of the shell $x_0=R/M$.