For extremal E2MD black holes, the coupling relation b=-1/a makes the long-range force between any two charge configurations vanish, with attraction on one side and repulsion on the other in every analytically controlled regime.
On the interactions and equilibrium between Einstein-Maxwell-Dilaton black holes
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abstract
We study the interactions and the conditions for the equilibrium of forces between generic non-rotating black holes of the Einstein-Maxwell-Dilaton (EMD) theory. We study known (and some new) solutions of the time-symmetric initial-data problem escribing an arbitrary number of those black holes, some of them with primary scalar hair. We show how one can distinguish between initial data corresponding to dynamical situations in which the black holes (one or many) are not in equilibrium and initial data which are just constant-time slices of a static solution of the full equations of motion describing static black holes using (self-)interaction energies. For a single black hole, non-vanishing self-interaction energy is always related to primary scalar hair and to a dynamical black hole. Removing the self-interaction energies in multi-center solutions we get interaction energies related to the attractive and repulsive forces acting on the black holes. As shown by Brill and Lindquist, for widely separated black holes, these take the standard Newtonian and Coulombian forms plus an additional interaction term associated with the scalar charges which is attractive for like charges.
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Mass and Force Relations for Extremal E2MD Black Holes
For extremal E2MD black holes, the coupling relation b=-1/a makes the long-range force between any two charge configurations vanish, with attraction on one side and repulsion on the other in every analytically controlled regime.