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arXiv 0908.2957gr-qchep-th
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膜-黑洞系统的曲率修正和拓扑变化跃迁:微扰方法

Curvature corrections and topology change transition in brane-black hole systems: A perturbative approach

Viktor G. Czinner, Antonino Flachi

摘要:

我们考虑曲率修正静态,轴对称的Dirac-Nambu-Goto膜嵌入到球对称黑洞时空与任意数量的维度。由于在有效膜作用量中,次高阶修正是膜厚度l的二次方,我们在l^2中采用线性微扰方法。扰动是一般意义上说,他们不限于Rindler区,也不近临界解的未扰动系统。结果发现,在微扰系统中存在一种意想不到的不对称性,在膜不穿过黑洞视界的构型中,如果膜的时空维数D>3,微扰方法不能得到正则解。然而,这个条件并不适用于视界交叉解。因此,我们认为,所提出的微扰方法打破了亚临界型解决方案的轴附近的系统D>3。然而,我们可以在D=2或3的情况下讨论拓扑变化的相变,即当膜分别是1维弦或2维片时。对于一般情况,应寻求一种不同的、非扰动的方法。基于从赤道组态准静态演化而来的膜的能量性质,我们给出了D=3膜的相变结果。据发现,小的厚度扰动不修改的过渡的顺序,即它仍然是第一阶的情况下消失的厚度。

英文摘要:

We consider curvature corrections to static, axisymmetric Dirac-Nambu-Goto membranes embedded into a spherically symmetric black hole spacetime with arbitrary number of dimensions. Since the next to leading order corrections in the effective brane action are quadratic in the brane thickness l, we adopt a linear perturbation approach in l^2. The perturbations are general in the sense that they are not restricted to the Rindler zone nor to the near-critical solutions of the unperturbed system. As a result, an unexpected asymmetry in the perturbed system is found. In configurations, where the brane does not cross the black hole horizon, the perturbative approach does not lead to regular solutions if the number of the brane's spacetime dimensions D>3. This condition, however, does not hold for the horizon crossing solutions. Consequently we argue that the presented perturbative approach breaks down for subcritical type solutions near the axis of the system for D>3. Nevertheless, we can discuss topology-changing phase transitions in cases when D=2 or 3, i.e. when the brane is a 1-dimensional string or a 2-dimensional sheet, respectively. For the general case, a different, non-perturbative approach should be sought. Based on the energy properties of those branes that are quasi-statically evolved from the equatorial configuration, we illustrate the results of the phase transition in the case of a D=3 brane. It is found that small thickness perturbations do not modify the order of the transition, i.e. it remains first order just as in the case of vanishing thickness.

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