2015
DOI: 10.1007/jhep04(2015)096
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The Renormalization Group flow of unimodular f(R) gravity

Abstract: Unimodular gravity is classically equivalent to General Relativity. This equivalence extends to actions which are functions of the curvature scalar. At the quantum level, the dynamics could differ. Most importantly, the cosmological constant is not a coupling in the unimodular action, providing a new vantage point from which to address the cosmological constant fine-tuning problem. Here, a quantum theory based on the asymptotic safety scenario is studied, and evidence for an interacting fixed point in unimodul… Show more

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Cited by 129 publications
(108 citation statements)
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References 111 publications
(184 reference statements)
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“…In fact, not only the precise location of the NGFP is regulator dependent (as expected), but also the value of the critical exponents depends on the truncation strategy employed to solve the flow equation [12,50]. Moreover recent investigations based on unimodular gravity [51], and general arguments [52] suggest that the critical exponents are indeed real [53,54].…”
Section: Basic Formalismmentioning
confidence: 57%
“…In fact, not only the precise location of the NGFP is regulator dependent (as expected), but also the value of the critical exponents depends on the truncation strategy employed to solve the flow equation [12,50]. Moreover recent investigations based on unimodular gravity [51], and general arguments [52] suggest that the critical exponents are indeed real [53,54].…”
Section: Basic Formalismmentioning
confidence: 57%
“…We recall that in the case m = −1/d the correspondence between g µν and γ µν is not invertible, so that the calculation presented here cannot be strictly applied in that case. This case has been considered from different viewpoints in [39][40][41][42][43][44]. Our results are a strong motivation to further investigate the quantum properties of this theory.…”
Section: Discussionmentioning
confidence: 81%
“…4.3 we used the generalised Legendre transform relation (33) to study the RG evolution of the corresponding exact solution U (y, t) to the Wilson/Polchinski LPA flow equation (6). Here the high temperature fixed point is given by a genuine fixed point of the flow, and this 'compactification' leads to better control of the corresponding quantised couplings h 2n (t) in the expansion (32).…”
Section: Discussionmentioning
confidence: 99%
“…The exact solution U (y, t) of the flow equation (6) with this boundary condition, is then given by (33).…”
Section: Couplings In the Wilsonian Effective Actionmentioning
confidence: 99%
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