Gravity solutions for the D1-D5 system with angular momentum

By O. Lunin, J. Maldacena, Liat Maoz. 2002

319 citations recorded by the source corpus.

We construct a large family of supergravity solutions that describe BPS excitations on AdS_3 x S^3 with angular momentum on S^3. These solutions take into account the full backreaction on the metric. We find that as we increase the energy of the excitation, the energy gap to the next non-BPS excitation decreases. These solutions can be viewed as Kaluza-Klein monopole ``supertubes'' which are completely non-singular geometries. We also make some remarks on supertubes in general.

Subfields: Astronomy and Astrophysics, Nuclear and High Energy Physics

View Paper: https://www.semanticscholar.org/paper/1ccfec01821351181710fc0c2a97436143d5d57a

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Citations in the corpus

Plumbing the Abyss: Black ring microstates (2007, background): “These calculations have been very successful both for two-charge solutions [1,3], and for simple three-charge solutions [17].”
Black holes as effective geometries (2008, background): “In [7] it was shown that the geometries corresponding to a classical curve are regular provided |F′(s)| is different from 0 and the curve is not self-intersecting.”
Global structure of five-dimensional fuzzballs (2013, background): “Mathur and collaborators went on to demonstrate that these fuzzball geometries could reproduce many of the properties of BPS black holes and of near-BPS black holes (see [1, 5, 6] for further discussion of this).”
The Search for a Holographic Dual to AdS(3)xS(3)xS(3)xS(1) (2004, background): “It is possible that these states correspond to conical defect geometries smoothed out into supertubes, along the lines described in [27].”
Bubbling supertubes and foaming black holes (2005, background): “However, based on the microscopic description of supertubes [35,36,18] we expect the solutions that correspond to multiple supertubes to be dual to CFT states with longer effective strings than the solutions that come from only one supertube.”
Supersymmetric black rings and three-charge supertubes (2004, background): “at the non-singular, horizon-free supergravity solutions describing these objects are in one-to-one correspondence with the Ramond-sector ground states of the supersymmetric D1-D5 string intersection [9, 10, 11]. It has been conjectured that supergravity solutions for three-charge supertubes might s”
Nonsupersymmetric smooth geometries and D1-D5-P bound states (2005, unknown): “It has been shown in [34] that the general supersymmetric solution in minimal six-dimensional supergravity could be written as a fibration over a four-dimensional hyper-K¨ahler base, and writing the supersymmetric two-charge solutions in this form played an important role in understanding the relati”
Fuzzballs with internal excitations (2007, methodology): “1 Introduction Over the last few years an interesting new proposal for the gravitational nature of black hole microstates has emerged [1, 2, 3]; see also [4, 5, 6], and [7].”
Adding momentum to D1-D5 system (2004, methodology): “It is interesting that for a somewhat simpler system which has only two charges (D1 and D5, but no momentum), one can actually construct the geometries corresponding to all microscopic states [5, 6].”
The Phase Structure of Higher-Dimensional Black Rings and Black Holes (2007, background): “These integrals take simple forms only when n is odd [41], while for even n they involve elliptic functions [42].”
One Ring to Rule Them All ... and in the Darkness Bind Them (2004, background): “Unlike the two-charge supertube solutions [8, 24, 25 , 26], these solutions cannot be found by usual solution generating techniques because the three charges can be generically dissolved into fluxes (as in the Klebanov–Strassler solution [21]).”