2018
DOI: 10.1088/1361-6382/aabaa0
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Infinite order quantum-gravitational correlations

Abstract: A new approximation scheme for nonperturbative renormalisation group equations for quantum gravity is introduced. Correlation functions of arbitrarily high order can be studied by resolving the full dependence of the renormalisation group equations on the fluctuation field (graviton). This is reminiscent of a local potential approximation in O(N)-symmetric field theories. As a first proof of principle, we derive the flow equation for the "graviton potential" induced by a conformal fluctuation and corrections i… Show more

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Cited by 41 publications
(29 citation statements)
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“…Here we used the symmetry in the two φ-fields to exchange the indices 2 and 3. By comparing (64) to (46) and (48), we see that split symmetry entails a specific relation between the form factors appearing in the vertex expansion. The (φφ)-vertex receives contributions from the scalar kinetic term only, and anticipating this we deliberately chose the same name for the two functions.…”
Section: Identities For Split-symmetric Verticesmentioning
confidence: 99%
“…Here we used the symmetry in the two φ-fields to exchange the indices 2 and 3. By comparing (64) to (46) and (48), we see that split symmetry entails a specific relation between the form factors appearing in the vertex expansion. The (φφ)-vertex receives contributions from the scalar kinetic term only, and anticipating this we deliberately chose the same name for the two functions.…”
Section: Identities For Split-symmetric Verticesmentioning
confidence: 99%
“…However, in the latter case the value of g 1 will change sign, and thus the solution becomes unphysical. If one uses now the type-II regulator for the fermions there will be a critical value of N D where g 1 becomes positive, for the solution (16) this value is N D = 14.1 whereas for the solution (17) it is N D = 12.9. If these values are exceeded the minimum turns to a maximum (but stays at the same location) and the values of g 1 and g 2 change sign.…”
Section: Global Solutions For Fixed Functions 321 Global Quadraticmentioning
confidence: 99%
“…For the solution (17) one obtains an interest- Table 1: Quadratic solutions for the fixed function with different matter content derived from the pure gravity solution (16). Table 2: Quadratic solution for the fixed function with different matter content derived from the pure gravity solution (17).…”
Section: Global Solutions For Fixed Functions 321 Global Quadraticmentioning
confidence: 99%
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“…Notwithstanding, the pseudo-spectral method using Chebyshev rational functions [130][131][132] has proved to be a versatile and robust tool to obtain a solution of arbitrary accuracy, at least in principle. As an example from the FRG context, it has been used successfully to obtain high-accuracy solutions of effective potentials for various model systems before 68,89,90,94,[133][134][135][136] . We will therefore expand the couplings and the anomalous dimension function as a series of Chebyshev rational functions R n (n = 0, 1, .…”
Section: A Solution Strategymentioning
confidence: 99%