1111.1897 (S. Kalyana Rama)
S. Kalyana Rama
We solve D = n + m + 2, m \ge 2, n \ge 1, dimensional vacuum Einstein's
equations for static, brane--like solutions. The general solution depends on
f(r) and F(r), and the constants (a_0, a_i, M_\infty) obeying a_0 + \sum_i a_i
= 1/2 and M_\infty > 0 . For 2 a_0 = 1 and a_i = 0, standard black n-brane
solution e^F = f = 1 - \frac{M_\infty} {r^{m - 1}} follows.
For a_0^2 + \sum_i a_i^2 > 1/4, the solutions have novel properties : as r
decreases from \infty to 0, {\bf (i)} f decreases from 1, reaches a minimum,
and increases to \infty, remaining strictly positive; {\bf (ii)} e^F decreases
monotonically from 1 to 0; and {\bf (iii)} the `mass' function M = r^{m - 1} (1
- f) decreases monotonically from M_\infty to - \infty . All metric components
remain non zero and finite for 0 < r \le \infty, hence there is no horizon or
singularity in this range. The presence of the n-dimensional space is crucial
for these properties. Such solutions may be naturally anticipated if Mathur's
fuzzball proposal for black holes is correct.
View original:
http://arxiv.org/abs/1111.1897
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