1977
DOI: 10.1103/physrevd.16.953
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Renormalization of higher-derivative quantum gravity

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Cited by 2,501 publications
(3,525 citation statements)
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“…1 This theory is important because in four dimensions it is power-counting renormalizable [5] and asymptotically free [6][7][8][9][10]. In spite of these appealing 1 There has been recently some progress on theories that contain more than four, and possibly infinitely many derivatives [2][3][4].…”
Section: Introductionmentioning
confidence: 99%
“…1 This theory is important because in four dimensions it is power-counting renormalizable [5] and asymptotically free [6][7][8][9][10]. In spite of these appealing 1 There has been recently some progress on theories that contain more than four, and possibly infinitely many derivatives [2][3][4].…”
Section: Introductionmentioning
confidence: 99%
“…It is worth clarifying that the decoupled equations are not the background field equations in the R + f (GB) frame where the Friedmann equation (the 00-field equation) contains third derivatives of the metric. As discussed in [45], the cancellation of fourth order derivatives in the decoupled equations is a necessary condition to have a theory free from massive spin-2 gravitons (ghosts) [24,41,42,44,45]. The condition imposes for us some relations between the parameters that we can use in order to combine R and R1.…”
Section: Higher-order Gravity Models Based On Minimal Setsmentioning
confidence: 99%
“…The first example we consider is where the function is that of the pure GB invariant given by, e.g. [24,41,44,45], (R 2 /6−8R1) . In the first order phase portrait of the coordinate plane (x, v), we find an accelerating attractor with the scale factor a(t) evolving as t p where p = 5.…”
Section: Higher-order Gravity Models Based On Minimal Setsmentioning
confidence: 99%
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