2014
DOI: 10.1103/physrevd.89.065005
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Topological solutions in ungauged supergravity

Abstract: A new general class of solutions of ungauged four-dimensional supergravity, in one-to-one correspondence with spherically symmetric, static black-hole solutions and Lifshitz solutions with hyperscaling violation is studied. The causal structure of the space-time is then elucidated.

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Cited by 8 publications
(16 citation statements)
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References 56 publications
(84 reference statements)
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“…These constraints are satisfied if n = 1 + δ with δ ≥ 0. In spite of the experimental bounds on the exponent n, R n gravity has been the focus of much work aiming at exploring the possible phenomenology of f (R) gravity and many phase space analyses for R n cosmology are available in the literature [91,92,93,94,95,96,97,98,99,100,101,102,103,104,105,106,107,108,109] (see [113] for a phase space picture of general f (R) cosmology analogous to that of the previous section). Moreover, in strong curvature regimes in the early universe, in which the present-day Solar System constraints do not apply, Starobinsky-like inflation [114] corresponding to f (R) = R + µR 2 is well approximated by f (R) ≃ µR 2 .…”
Section: A Phase Space Interpretationmentioning
confidence: 99%
“…These constraints are satisfied if n = 1 + δ with δ ≥ 0. In spite of the experimental bounds on the exponent n, R n gravity has been the focus of much work aiming at exploring the possible phenomenology of f (R) gravity and many phase space analyses for R n cosmology are available in the literature [91,92,93,94,95,96,97,98,99,100,101,102,103,104,105,106,107,108,109] (see [113] for a phase space picture of general f (R) cosmology analogous to that of the previous section). Moreover, in strong curvature regimes in the early universe, in which the present-day Solar System constraints do not apply, Starobinsky-like inflation [114] corresponding to f (R) = R + µR 2 is well approximated by f (R) ≃ µR 2 .…”
Section: A Phase Space Interpretationmentioning
confidence: 99%
“…In contradistinction for regular geometry with an interior wormhole spacetime, r 0 ≤ r ≤ R, and a Schwarzschildlike vacuum, r h < R ≤ r < ∞, at a junction interface. In addition, the junction conditions in this theory have been worked out [86].…”
Section: V1 Field Equations With Conformal Symmetry In Teleparallelmentioning
confidence: 99%
“…Probing properties of the dark energy is important, and it has been studied in the standard cosmology or the several modified gravity theories [59][60][61][62][63][64][65][66][67][68][69][70][71][72][73][74][75]. Next we investigate the properties of geometrical dark energy in this GBD theory, and analyze the effects of the BD scalar field.…”
Section: Effective State Parameter Of Geometrical Dark Energy In mentioning
confidence: 99%
“…Studies on the modified gravity theories of GR have been always the hot area. Several modified gravity theories have been widely studied [1][2][3][4][5][6], especially two simple modifications to GR: the f (R) theory [7,8] and the Brans-Dicke (BD) theory [9].…”
Section: Introductionmentioning
confidence: 99%