We investigate the structure of smooth and horizonless microstate geometries in six dimensions, in the spirit of the five-dimensional analysis of Gibbons and Warner [arXiv: 1305.0957]. In six dimensions, which is the natural setting for horizonless geometries with the charges of the D1-D5-P black hole, the natural black objects are strings and there are no Chern-Simons terms for the tensor gauge fields. However, we still find that the same reasoning applies: in absence of horizons, there can be no smooth stationary solutions without non-trivial topology. We use topological arguments to describe the Smarr formula in various examples: the uplift of the five-dimensional minimal supergravity microstates to six dimensions, the two-charge D1-D5 m...
We construct a discrete family of smooth non-supersymmetric three charge geometries carrying D1 bran...
We use the formalism of Generalised Geometry to characterise in general the supersymmetric backgroun...
International audienceWe find the first smooth bubbling microstate geometries with non-Abelian field...
We investigate the structure of smooth and horizonless microstate geometries in six dimensions, in t...
The equations underlying all supersymmetric solutions of six-dimensional minimal ungauged supergravi...
v2: Eqs. (2.1), (2.39) corrected, references added. v3: minor correctionsInternational audienceThe e...
Abstract We present the construction of several microstate geometries of the supersymmetric D1-D5-P ...
International audienceWe systematically study all supersymmetric solutions of six-dimensional (2, 0)...
5 pages, 1 figureInternational audienceWe construct the first family of horizonless supergravity sol...
Abstract We outline a systematic procedure to obtain horizonless microstate geometries that have the...
We describe and study families of BPS microstate geometries, namely, smooth, horizon-less asymptotic...
We construct the first family of horizonless supergravity solutions that have the same mass, charges...
We construct a discrete family of smooth non-supersymmetric three charge geometries carrying D1 bran...
We use the formalism of Generalised Geometry to characterise in general the supersymmetric backgroun...
International audienceWe find the first smooth bubbling microstate geometries with non-Abelian field...
We investigate the structure of smooth and horizonless microstate geometries in six dimensions, in t...
The equations underlying all supersymmetric solutions of six-dimensional minimal ungauged supergravi...
v2: Eqs. (2.1), (2.39) corrected, references added. v3: minor correctionsInternational audienceThe e...
Abstract We present the construction of several microstate geometries of the supersymmetric D1-D5-P ...
International audienceWe systematically study all supersymmetric solutions of six-dimensional (2, 0)...
5 pages, 1 figureInternational audienceWe construct the first family of horizonless supergravity sol...
Abstract We outline a systematic procedure to obtain horizonless microstate geometries that have the...
We describe and study families of BPS microstate geometries, namely, smooth, horizon-less asymptotic...
We construct the first family of horizonless supergravity solutions that have the same mass, charges...
We construct a discrete family of smooth non-supersymmetric three charge geometries carrying D1 bran...
We use the formalism of Generalised Geometry to characterise in general the supersymmetric backgroun...
International audienceWe find the first smooth bubbling microstate geometries with non-Abelian field...