1,417 research outputs found
Non-Supersymmetric Attractors
We consider theories with gravity, gauge fields and scalars in
four-dimensional asymptotically flat space-time. By studying the equations of
motion directly we show that the attractor mechanism can work for
non-supersymmetric extremal black holes. Two conditions are sufficient for
this, they are conveniently stated in terms of an effective potential involving
the scalars and the charges carried by the black hole. Our analysis applies to
black holes in theories with supersymmetry, as well as
non-supersymmetric black holes in theories with supersymmetry.
Similar results are also obtained for extremal black holes in asymptotically
Anti-de Sitter space and in higher dimensions.Comment: 55 pages, LaTeX, 7 eps figures. v3: references and some additional
comments added, minor correction
Characterization of almost -eigenfunctions of the Laplace-Beltrami operator
In \cite{Roe} Roe proved that if a doubly-infinite sequence of
functions on satisfies and for
all and , then where
and are real constants. This result was extended to by
Strichartz \cite{Str} where is substituted by the Laplacian on .
While it is plausible to extend this theorem for other Riemannian manifolds or
Lie groups, Strichartz showed that the result holds true for Heisenberg groups,
but fails for hyperbolic 3-space. This negative result can be indeed extended
to any Riemannian symmetric space of noncompact type. We observe that this
failure is rooted in the -dependance of the -spectrum of the Laplacian
on the hyperbolic spaces. Taking this into account we shall prove that for all
rank one Riemannian symmetric spaces of noncompact type, or more generally for
the harmonic groups, the theorem actually holds true when uniform
boundedness is replaced by uniform "almost boundedness". In addition we
shall see that for the symmetric spaces this theorem is capable of
characterizing the Poisson transforms of functions on the boundary, which
some what resembles the original theorem of Roe on .Comment: 30 page
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