No Run Gravity

dc.contributor.authorEric V. Linder
dc.date.accessioned2025-08-13T06:17:00Z
dc.date.available2025-08-13T06:17:00Z
dc.date.issued2019
dc.description.abstractConsidering the dark energy/gravity landscape if next generation surveys of galaxies, cosmic microwave background radiation, and gravitational waves do not find clear modification of gravity, we develop No Run Gravity as a counterexample to the conclusion that this would imply general relativity with an expansion history described by an equation of state 𝑤 ( 𝑧 ) w(z). No Run Gravity is a cubic Horndeski theory with a constant Planck mass, no gravitational slip, and no modification of gravitational waves, but a rich phenomenology beyond 𝑤 ( 𝑧 ) w(z). We calculate the evolution of gravitational strength, sound speed, and cosmic growth within the theory and project sensitivities for upcoming DESI redshift space distortion data.
dc.identifier.citationLinder, E. V. (2019). No Run Gravity. arXiv preprint arXiv:1903.02010. — Note: subsequently framed within the "Limited Modified Gravity" framework
dc.identifier.urihttps://nur.nu.edu.kz/handle/123456789/9196
dc.language.isoen
dc.publisherarXiv
dc.rightsAttribution-NonCommercial-ShareAlike 3.0 United Statesen
dc.rights.urihttp://creativecommons.org/licenses/by-nc-sa/3.0/us/
dc.subjectmodified gravity
dc.subjectHorndeski theory
dc.subjectPlanck mass constant
dc.subjectgravitational slip
dc.subjectcosmic growth
dc.subjectNo Run Gravity
dc.subjecttype of access: open access
dc.titleNo Run Gravity
dc.typeArticle

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