Orthodox quantization of Einstein's gravity: might its unrenormalizability be technically fathomable and physically innocuous?
Steven Kenneth Kauffmann

TL;DR
This paper discusses the nonanalytic nature of quantum gravity in G, its implications for renormalizability, and suggests that classical gravity coupled with quantized fields might be a practical approach due to the smallness of hG.
Contribution
It proposes that the nonrenormalizability of quantum gravity is a consequence of nonanalyticity in G and advocates for a semiclassical approach coupling classical gravity with quantized matter fields.
Findings
Quantum gravity amplitudes are nonanalytic in G at G=0.
Perturbation expansions in G are divergent and unrenormalizable.
Classical gravity treatment is sufficient due to the smallness of hG.
Abstract
Many physical constants related to quantized gravity, e.g., the Planck length, mass, curvature, stress-energy, etc., are nonanalytic in G at G=0, and thus have expansions in powers of G whose terms are progressively more divergent with increasing order. Since the gravity field's classical action is inversely proportional to G, the path integral for gravity-field quantum transition amplitudes shows that these depend on G only through the product hG, and are nonanalytic in G at G=0 for the same reason that all quantum transition amplitudes are nonanalytic in h at h=0, namely their standard oscillatory essential singularity at the classical "limit". Thus perturbation expansions in powers of G of gravity-field transition amplitudes are also progressively more divergent with increasing order, and hence unrenormalizable. While their perturbative treatment is impossible, the exceedingly small…
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Taxonomy
TopicsCosmology and Gravitation Theories · Relativity and Gravitational Theory · Noncommutative and Quantum Gravity Theories
