Local gravity theories in conformal superspace

被引:0
作者
Gomes, Henrique [1 ]
机构
[1] Perimeter Inst Theoret Phys, 31 Caroline St, Waterloo, ON N2L 2Y5, Canada
关键词
The York conformal method for the IVP GR; 3-dimensional conformal geometry (Cotton tensor); Problem time; Horava-Lifschitz; Hypersurface deformation algebra; BRST in QG; INITIAL-VALUE PROBLEM; GENERAL-RELATIVITY; QUANTUM-THEORY; MANIFOLD; DECOMPOSITION; EXISTENCE; GEOMETRY; METRICS; TENSOR;
D O I
10.1016/j.aop.2018.05.014
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
The conformal method for the initial value formulation of GR is one of the most powerful and widely used tools in both analytical studies and numerical simulations of solutions. As is well-known, it exploits a hidden spatial conformal symmetry that can be extracted from the equations. But why conformal symmetry? Motivated by these questions and by well-known obstacles to quantum gravity, I look for the most general geometrodynamical symmetries compatible with a reduced physical configuration space for metric gravity. I argue that they are indeed spatial conformal diffeomorphisms. The next question is: what sort of theories most naturally incorporate this symmetry? Demanding locality for an action for metric gravity compatible with these principles determines the allowed operators, both for the purely gravitational part as well as matter couplings. The symmetries guarantee that there are two gravitational propagating physical degrees of freedom, but no explicit refoliation-invariance. The simplest such system has a geometric interpretation as a geodesic model in infinite-dimensional conformal superspace. One example of solution to the equations of motion corresponds to a static Bianchi IX spatial ansatz. The unique coupling to electromagnetism forces the electromagnetic equations to be hyperbolic, enabling us to "build" a standard space-time causal structure. There are, however, deviations from the standard Maxwell equations when space-time anisotropies become too large. Regarding quantization, with the geometric interpretation and the lack of refoliation invariance, the path integral treatment of the symmetries becomes much less involved than the similar approaches to GR. The symmetries form an (infinite-dimensional) Lie algebra, and no BFV treatment is necessary. Moreover, one can use gauge-invariant variational principles for selecting the boundary conditions of the path integral. We find that the propagator around the homogeneous solution has up to 6th order spatial derivatives, giving it plausible regularization properties as in Horava-Lifschitz. (C) 2018 Elsevier Inc. All rights reserved.
引用
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页码:423 / 457
页数:35
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