论文标题

五维引力brane-world模型:黑弦和黑洞的解决方案

Five-dimensional gravitational brane-world models: Solutions for black strings and black holes

论文作者

Nakas, Theodoros

论文摘要

储层计算是预测湍流的有力工具,其简单的架构具有处理大型系统的计算效率。然而,其实现通常需要完整的状态向量测量和系统非线性知识。我们使用非线性投影函数将系统测量扩展到高维空间,然后将其输入到储层中以获得预测。我们展示了这种储层计算网络在时空混沌系统上的应用,该系统模拟了湍流的若干特征。我们表明,使用径向基函数作为非线性投影器,即使只有部分观测并且不知道控制方程,也能稳健地捕捉复杂的系统非线性。最后,我们表明,当测量稀疏、不完整且带有噪声,甚至控制方程变得不准确时,我们的网络仍然可以产生相当准确的预测,从而为实际湍流系统的无模型预测铺平了道路。

In the context of this dissertation, we study the emergence of black-string and black-hole solutions in the framework of five-dimensional braneworld models. The main motivation for studying such theories stems from the Randall-Sundrum model, which was formulated by Lisa Randall and Raman Sundrum back in 1999. We investigate thoroughly the physical characteristics of analytic solutions which concern both black strings and five-dimensional localized black holes. To be more precise, the black-string solutions emerge in the context of a five-dimensional scalar-tensor theory, where the brane line-element is found to describe a Schwarzschild-(anti-)de Sitter spacetime. The cases of de Sitter, anti-de Sitter and Minkowski branes are examined separately and in great detail. As far as the five-dimensional black holes are concerned, at first, we present an "algorithm" that one may use in order to construct from first principles the geometry of analytic and exponentially localized five-dimensional braneworld black holes. In each case, the point-like singularity of the black hole lies entirely on the 3-brane, while its event horizon is exponentially localized close to the 3-brane thus exhibiting a pancake shape. In the first case, the induced line-element on the brane assumes the form of the Schwarzschild solution while the bulk geometry is effectively AdS$_5$ outside the horizon. In the second case, the induced brane geometry is described by the Reissner-Nordström-(A)dS line-element, where a careful classification of the horizons takes place as well. In both cases, the derived geometry is supported by an anisotropic fluid in the bulk described only by two independent components, the energy density and tangential pressure, whereas no matter needs to be introduced on the brane for its consistent embedding in the bulk.

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