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M. Cvetic et al
1999
Earlier work this paper cites.
M. J. Duff and J. T. Liu, “Anti-de Sitter black holes in gauged N = 8 supergravity,” Nucl. Phys
1999
Earlier work this paper cites.
H. A. Chamblin and H. S. Reall, “Dynamic dilatonic domain walls,” Nucl. Phys
1999
Earlier work this paper cites.
M. Cvetic, H. Lu, and C. N. Pope, “Geometry of the embedding of supergravity scalar manifolds in D = 11 and D = 10,” Nucl. Phys
2000
Earlier work this paper cites.
S. S. Gubser, “Curvature singularities: The Good, the bad, and the naked,” Adv. Theor. Math. Phys
2000
Earlier work this paper cites.
N. Kundu, P. Narayan, N. Sircar, and S. P. Trivedi, “Entangled Dilaton Dyons,” JHEP
Original
2008
Earlier work this paper cites.
O. Aharony, O. Bergman, D. L. Jafferis, and J. Maldacena, “N=6 superconformal Chern-Simons-matter theories, M2-branes and their gravity duals,” JHEP
Original
2008
Earlier work this paper cites.
T. Azeyanagi, W. Li, and T. Takayanagi, “On String Theory Duals of Lifshitz-like Fixed Points,” JHEP
Original
2009
Earlier work this paper cites.
C. Charmousis, B. Goutéraux, B. Kim, E. Kiritsis, and R. Meyer, “Effective Holographic Theories for low-temperature condensed matter systems,” JHEP
Original
2010
Earlier work this paper cites.
S. S. Gubser, S. S. Pufu, and F. D. Rocha, “Quantum critical superconductors in string theory and M- theory,” Phys. Lett
Original
2010
Earlier work this paper cites.
D. Mateos and D. Trancanelli, “The anisotropic N=4 super Yang-Mills plasma and its instabilities,” Phys.Rev.Lett
Original
2011
Earlier work this paper cites.
D. Mateos and D. Trancanelli, “Thermodynamics and Instabilities of a Strongly Coupled Anisotropic Plasma,” JHEP
Original
2011
Earlier work this paper cites.
T. Faulkner, N. Iqbal, H. Liu, J. McGreevy, and D. Vegh, “Holographic non-Fermi liquid fixed points,” Phil. Trans. Roy. Soc
Original
2011
Earlier work this paper cites.

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2017

Boomerang RG flows in M-theory with intermediate scaling

Donos, Aristomenis, Gauntlett, Jerome P., Rosen, Christopher et al.

Understand

We construct novel RG flows of D=11 supergravity that asymptotically approach $AdS_4\times S^7$ in the UV with deformations that break spatial translations in the dual field theory.

In the IR the solutions return to exactly the same $AdS_4\times S^7$ vacuum, with a renormalisation of relative length scales, and hence we refer to the flows as `boomerang RG flows'.
For sufficiently large deformations, on the way to the IR the solutions also approach two distinct intermediate scaling regimes, each with hyperscaling violation.
The first regime is Lorentz invariant with dynamical exponent $z=1$ while the second has $z=5/2$.