Gravity theory through affine spheres

8th International Workshop DICE2016: Spacetime - Matter - Quantum Mechanics

物理学;力学

Minguzzi, E.^1

Dipartimento di Matematica e Informatica U. Dini, Università degli Studi di Firenze, Via S. Marta 3, Firenze

I-50139, Italy^1

关键词: Affine parameters;    Cone structures;    Differential geometry;    Dispersion relations;    Dynamical variables;    General Relativity;    Space-time continuum;    Space-time volume;   

Others  :  https://iopscience.iop.org/article/10.1088/1742-6596/880/1/012005/pdf
DOI  :  10.1088/1742-6596/880/1/012005

学科分类：力学，机械学

来源: IOP

【 摘 要 】

In this work it is argued that in order to improve our understanding of gravity and spacetime our most successful theory, general relativity, must be destructured. That is, some geometrical assumptions must be dropped and recovered just under suitable limits. Along this line of thought we pursue the idea that the roundness of the light cone, and hence the isotropy of the speed of light, must be relaxed and that, in fact, the shape of light cones must be regarded as a dynamical variable. Mathematically, we apply some important results from affine differential geometry to this problem, the idea being that in the transition we should preserve the identification of the spacetime continuum with a manifold endowed with a cone structure and a spacetime volume form. To that end it is suggested that the cotangent indicatrix (dispersion relation) must be described by an equation of Monge-Ampère type determining a hyperbolic affine sphere, at least whenever the matter content is negligible. Non-relativistic spacetimes fall into this description as they are recovered whenever the center of the affine sphere is at infinity. In the more general context of Lorentz-Finsler theories it is shown that the lightlike unparametrized geodesic flow is completely determined by the distribution of light cones. Moreover, the transport of lightlike momenta is well defined though there could be no notion of affine parameter. Finally, we show how the perturbed indicatrix can be obtained from the perturbed light cone.