2013
DOI: 10.3390/galaxies2010001
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Galaxy Rotation Curves in Covariant Hořava-Lifshitz Gravity

Abstract: Using the multiplicity of solutions for the projectable case of the covariant extension of Hořava-Lifshitz gravity, we show that an appropriate choice for the auxiliary field allows for an effective description of galaxy rotation curves. This description is based on static and spherically symmetric solutions of covariant Hořava-Lifshitz gravity and does not require Dark Matter.

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Cited by 4 publications
(3 citation statements)
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“…Even though dark matter is by far the most accepted explanation for the resolution to the galaxy rotation problem, there have been other proposals with varying degrees of success. Among them, the most popular ones involve certain modification of the laws of gravity, starting with the seminal works [94,95] and continuing with a large body of work that includes [96,97,98,99,100,101,102,103,104,105,106] and the recent additions [107,108,109,110,111,112].…”
Section: Rotation Curvesmentioning
confidence: 99%
“…Even though dark matter is by far the most accepted explanation for the resolution to the galaxy rotation problem, there have been other proposals with varying degrees of success. Among them, the most popular ones involve certain modification of the laws of gravity, starting with the seminal works [94,95] and continuing with a large body of work that includes [96,97,98,99,100,101,102,103,104,105,106] and the recent additions [107,108,109,110,111,112].…”
Section: Rotation Curvesmentioning
confidence: 99%
“…This covariant extension to HL has led to several studies, including spherically symmetric solutions [6] and their relevance to an alternative model for galaxy rotation curves [7], cosmological solutions [8], as well as theoretical and phenomenological consistency tests of the theory [9].…”
Section: Introductionmentioning
confidence: 99%
“…Spherically symmetric static spacetimes in the framework of the HL theory with U(1) symmetry with or without the projectabilty condition are studied systematically in [26,27,29,35,36,47,48]. In particular, the ADM variables for spherically symmetric spacetimes with the projectability condition take the forms…”
Section: Spherical Spacetimes Filled With a Fluidmentioning
confidence: 99%