We investigate continuously self-similar solutions of four-dimensional Einstein-Maxwelldilaton theory supported by charged null fluids. We work under the assumption of spherical symmetry and the dilaton coupling parameter a is allowed to be arbitrary. First, it is proved that the only such vacuum solutions with a time-independent asymptotic value of the dilaton necessarily have vanishing electric field, and thus reduce to Roberts' solution of the Einsteindilaton system. Allowing for additional sources, we then obtain Vaidya-like families of selfsimilar solutions supported by charged null fluids. By continuously matching these solutions to flat spacetime along a null hypersurface one can study gravitational collapse analytically. Capitalizing on this idea, we compute the critical exponent defining the power-law behavior of the mass contained within the apparent horizon near the threshold of black hole formation. For the heterotic dilaton coupling a = 1 the critical exponent takes the value 1/2 typically observed in similar analytic studies, but more generally it is given by γ = a 2 (1 + a 2 ) −1 . The analysis is complemented by an assessment of the classical energy conditions. Finally, and on a different note, we report on a novel dyonic black hole spacetime, which is a time-dependent vacuum solution of this theory. In this case, the presence of constant electric and magnetic charges naturally breaks self-similarity.
arXiv:1907.02715v1 [hep-th] 5 Jul 2019Gravitational collapse is the classical mechanism responsible for the formation of black holes in the universe. It occurs when the matter density is so high that gravitational attraction, the weakest of all known forces, dominates over all other forces of nature. It has been understood long ago that stellar-mass black holes can be formed when sufficiently massive stars exhaust their nuclear fuel [1]. Alternatively, primordial black holes may have formed in the early universe as the result of the gravitational collapse of cosmological density fluctuations [2], although there is currently no observational evidence for their existence.Once gravitational collapse sets in, typically it is not guaranteed that a black hole will form. This only occurs if the initial conditions are sufficiently 'strong' in some sense. Otherwise, the matter contracts without ever generating sufficiently high densities to produce an event horizon and then fully disperses, leaving behind flat space. This problem was first investigated by Christodoulou in a series of papers [3,4], taking a massless scalar field as the matter model. At the threshold between forming or not a black hole during gravitational collapse, critical phenomena arises. This was revealed by Choptuik in a seminal paper [5], which studied numerically the same problem previously considered by Christodoulou and which set much of the groundwork for the field that became known as critical collapse (see [6] for a review).Near the threshold of black hole formation Choptuik found universal behavior, emergent self-similarity, and t...