Abstract

We present a detailed description of N=2 stationary BPS multicenter black hole solutions for quadratic prepotentials with an arbitrary number of centers and scalar fields making a systematic use of the algebraic properties of the matrix of second derivatives of the prepotential, $\mathcal{S}$, which in this case is a scalar-independent matrix. In particular we obtain bounds on the physical parameter of the multicenter solution such as horizon areas and ADM mass. We discuss the possibility and convenience of setting up a basis of the symplectic vector space built from charge eigenvectors of the $\ssigma$, the set of vectors $(\Ppm q_a)$ with $\Ppm$ $\ssigma$-eigenspace proyectors. The anti-involution matrix $\mathcal{S}$ can be understood as a Freudenthal duality $\tilde{x}=\ssigma x$. We show that this duality can be generalized to "Freudenthal transformations" $$x\to \lambda\exp(\theta \ssigma) x= a x+b\tilde{x}$$ under which the horizon area, ADM mass and intercenter distances scale up leaving constant the fix point scalars. In the special case $\lambda=1$, "$\ssigma$-rotations", the transformations leave invariant the solution. The standard Freudental duality can be written as $\tilde x= \exp(\pi/2 \ssigma) x .$ We argue that these generalized transformations leave also invariant the general stringy extremal quartic form $\Delta_4$, $\Delta_4(x)= \Delta_4(\cos\theta x+\sin\theta\tilde{x})$.

Highlights

  • X → λ exp(θS)x = ax + bxunder which the horizon area, ADM mass and intercenter distances scale up leaving constant the scalars at the fixed points

  • We present a detailed description of N = 2 stationary BPS multicenter black hole solutions for quadratic prepotentials with an arbitrary number of centers and scalar fields making a systematic use of the algebraic properties of the matrix of second derivatives of the prepotential, S, which in this case is a scalar-independent matrix

  • We argue at the final section of this work that these generalized Freudenthal transformations leave invariant the entropy and other macroscopical quantities of quadratic prepotential theories and ∆4, the quartic invariant [33] appearing in the description of more general theories, 4d SUGRAs that arise from String and M-theory and the lowest order entropy of these theories

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Summary

General supersymmetric stationary solutions

We will use the properties of the stabilization matrix S to solve them in a purely algebraic way to obtain some properties and give some explicit expressions for the scalars at the fixed points For this purpose, we first establish some well-known properties of SN , S ≡ SF and define new matrices: some projector operators associated to them and their respective symplectic adjoints. SV = 2iSP−Im (V ) = 2P−Im (V ) = iV We find it convenient to define the adjoint operator S† of the matrix S, with respect to the symplectic bilinear product so that, for any vectors A, B ∈ W , we have. Any physical quantity (entropy, ADM mass, scalars at fixed points, intercenter distances, etc.) written in terms of these products (as it will clearly appear ) will automatically be scaled under the general transformations or invariant under the rotations.

Scalar fields at the fixed points
Behavior of the scalar field solutions
Intercenter distances and S-transformations
Near horizon and infinity geometry
Freudenthal duals and charge vector expansions
Summary and concluding remarks
Full Text
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