论文标题
球形对称广告中的新（原始）一组准正常模式黑洞空位
A new (original) set of Quasi-normal modes in spherically symmetric AdS black hole spacetimes
论文作者
论文摘要
从黑洞扰动理论中，通常通过施加Dirichlet或消失的能量磁通量边界条件来研究球形对称广告中的准正常模式（QNM）黑洞空位[1]。使用标量扰动案例和类似盒子的有效电位构建了该方法，当径向坐标接近无穷大时，径向方程倾向于无穷大。这些QNM与屏障样有效电位获得的QNM可以实现为不同的解决方案。但是，在某些情况下，可以在广告中存在类似屏障样的有效电位，而黑洞空位则存在。在这些情况下，这意味着当径向坐标分别进入事件范围和无穷大时，我们将通过纯粹的凹槽和纯粹的边界条件获得新的（原始）QNM。在ADS黑洞案例中获得这组QNM是本文的主要重点。
From black hole perturbation theory, quasi-normal modes (QNMs) in spherically symmetric AdS black hole spacetimes are usually studied with the Horowitz and Hubeny methods [1] by imposing the Dirichlet or vanishing energy flux boundary conditions. This method was constructed using the scalar perturbation case and box-like effective potentials, where the radial equation tends to go to infinity when the radial coordinate approaches infinity. These QNMs can be realized as a different set of solutions from those obtained by the barrier-like effective potentials. However, in some cases the existence of barrier-like effective potentials in AdS black hole spacetimes can be found. In these cases this means that we would obtain a new (original) set of QNMs by the purely ingoing and purely outgoing boundary conditions when the radial coordinate goes to the event horizon and infinity, respectively. Obtaining this set of QNMs in AdS black hole cases is the main focus of this paper.
