PHYS08200604018 Shamik Banerjee - Homi Bhabha National ...
PHYS08200604018 Shamik Banerjee - Homi Bhabha National ...
PHYS08200604018 Shamik Banerjee - Homi Bhabha National ...
Create successful ePaper yourself
Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.
Chapter 6<br />
Concluding Remarks<br />
Complete understanding of the microstates of an arbitrary black hole is one the motivations<br />
behind a quantum theory of grvity. String theory is the leading candidate for a quantum gravity<br />
theory and there is much progress in understanding the microscopics of supersymmetric black<br />
holes.<br />
In this thesis our aim was to calculate the microscopic degeneracy of Black holes, in N = 4<br />
superstring theory, which preserve 1 -th of the supersymmetries. The formula was known [7] for<br />
4<br />
black holes which carry charges (Q, P ) subject to the condition, g.c.d(Q ∧ P ) = 1 [20, 48, 63].<br />
We extended the result to black holes carrying arbitrary charge vectors. Although we could not<br />
provide a first principle derivation of the result, it was done after some time in the reference [85].<br />
There are some aspects of these formulae which require better understanding. We have<br />
already seen the appearance of the modular group of the genus two surface, namely Sp(2, Z).<br />
The partition function of the theory is given by a modular form of this group or one of its<br />
subgroups. But the appearance of Sp(2, Z) is not expected because it is not a symmetry<br />
group of the theory. The S-duality group is only a subgroup of this. The first step towards<br />
explaining this has been taken in [10, 18]. The contour prescription which we discussed in the<br />
introduction can also be derived [84] from the M-theory lift described in the last two papers.<br />
It will be very interesting to see how much more can be learned from this picture.<br />
97