Lifshitz solutions of D=10 and D=11 supergravity

By Aristomenis Donos, J. Gauntlett. 2010

169 citations recorded by the source corpus.

We construct infinite families of Lifshitz solutions of D = 10 and D = 11 supergravity with dynamical exponent z = 2. The new solutions are based on five-and seven-dimensional Einstein manifolds and are dual to field theories with Lifshitz scaling in 1+2 and 1+1 spacetime dimensions, respectively. When the Einstein spaces are Sasaki-Einstein, the solutions are supersymmetric.

Subfields: Astronomy and Astrophysics, Nuclear and High Energy Physics, Statistical and Nonlinear Physics

View Paper: https://www.semanticscholar.org/paper/f6f5a957395464af934198ec489fca07105c4d7d

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Citations in the corpus

Lifshitz solutions in supergravity and string theory (2010, methodology): “[8], the authors argue that their 10/11D Lifshitz compactifications can be supersymmetric when they are based on Sasaki-Einstein manifolds.”
Holographic Fermi and non-Fermi liquids with transitions in dilaton gravity (2011, unknown): “Third, the solution is somewhat analogous to Lifhsitz type solutions [30–33], however, in general the metric in the solution does not have any scaling symmetry.”
Holographic Quantum Matter (2016, unknown): “There is a large literature constructing Lifshitz spacetimes from consistent truncations of string theory, starting with [65; 210].”
Thermodynamics and instabilities of a strongly coupled anisotropic plasma (2011, methodology): “(2)Embeddings of Lifshitz geometries in string theory were constructed in [74, 75, 76, 77, 78, 79, 80, 81, 82].”
Boundary stress-energy tensor and Newton-Cartan geometry in Lifshitz holography (2013, methodology): “The model that we use can be obtained by dimensional reduction of the following 5dimensional action [57, 58, 62]”
Holographic entanglement entropy in Lovelock gravities (2011, unknown): “Recently, Lifshitz geometries have been embedded in string theory [79-82].”
Lifshitz holography (2015, unknown): “A systematic search for top down Lifshitz supergravity solutions was carried out in [29].”
Wrapped M5-branes, consistent truncations and AdS/CMT (2010, methodology): “However, Lif4(z = 2) solutions of type IIB and Lif3(z = 2) solutions of D = 11 supergravity were recently constructed in [36] and these were significantly extended in [ 37 ] where supersymmetric solutions were also presented (which should be stable).”
Aspects of holography for theories with hyperscaling violation (2012, background): “1 Such metrics have also been found as solutions in string theory, and supergravities which arise simply from string constructions, in [11–18].”
Torsional Newton–Cartan geometry and the Schrödinger algebra (2014, methodology): “developments: the work [10] which showed the usefulness of Newton{Cartan geometry in the eective eld theory description of the quantum Hall eect and the work [11,12], building forth on earlier work [13,14,15,16] and [17,18,19,20,21,22], which showed that the boundary geometry of a specic class of as”
Lifshitz scaling and hyperscaling violation in string theory (2012, methodology): “1 M2-branes with null deformations and D2-branes Null deformations of AdS4 × X(7) solutions obtained from near horizon regions of (extremal) M2-brane stacks in M-theory were discussed in [5, 6] to obtain z = 2 Lifshitz spacetimes in bulk 2 + 1-dimensions(4).”
Black holes and black branes in Lifshitz spacetimes (2011, background): “ifshitz geometries. Both formulations have their own virtues, but also their disadvantages. The formulation with massive gauge ﬁelds can be embedded in supergravity models and string compactiﬁcations [5, 26, 27, 28, 29, 16, 24], but as mentioned above, the study of black holes is mostly numerical or”