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Asymptotic Freedom in Renormalisable Gravity and Supergravity

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Quantum Gravity
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Abstract

Pure Einstein gravity is known to be non-renormalizable. Though the theory is one-loop finite on shell it probably possesses a divergent S-matrix starting from the two-loop order. The situation is even worse when ordinary matter is added. Quantizing matter fields in the classical metric background we already need bare curvature squared R2-terms in order to absorb the infinities. The possible was of improvement suggest themselves: (i) we may try to arrange all matter fields in a multiplet in order to cancel dangerous divergences. This is the way of supergravity known to be only partially successful at present (only one- and two-loop on shell finiteness was established); (ii) one can add the R2-terms to the Einstein langragian thus obtaining a manifestly renormalizable theory.

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© 1984 Plenum Press, New York

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Fradkin, E.S., Tseytlin, A.A. (1984). Asymptotic Freedom in Renormalisable Gravity and Supergravity. In: Markov, M.A., West, P.C. (eds) Quantum Gravity. Springer, Boston, MA. https://doi.org/10.1007/978-1-4613-2701-1_3

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  • DOI: https://doi.org/10.1007/978-1-4613-2701-1_3

  • Publisher Name: Springer, Boston, MA

  • Print ISBN: 978-1-4612-9678-2

  • Online ISBN: 978-1-4613-2701-1

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