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首页> 外文期刊>Geombinatorics >ON GEOMETRY OF FINSLER CAUSALITY: FOR CONVEX CONES, THERE IS NO AFFINE-INVARIANT LINEAR ORDER (SIMILAR TO COMPARING VOLUMES)
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ON GEOMETRY OF FINSLER CAUSALITY: FOR CONVEX CONES, THERE IS NO AFFINE-INVARIANT LINEAR ORDER (SIMILAR TO COMPARING VOLUMES)

机译:关于芬斯勒因果关系的几何:对于凸锥,没有仿射不变的线性阶(类似于比较体积)

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摘要

Some physicists suggest that to more adequately describe the causal structure of space-time, it is necessary to go beyond the usual pseudo-Riemannian causality, to a more general Finsler causality. In this general case, the set of all the events which can be influenced by a given event is, locally, a generic convex cone, and not necessarily a pseudo-Reimannian-style quadratic cone. Since all current observations support pseudo-Riemannian causality, Finsler causality cones should be close to quadratic ones. It is therefore desirable to approximate a general convex cone by a quadratic one. This cane be done if we select a hyperplane, and approximate intersections of cones and this hyperplane. In the hyperplane, we need to approximate a convex body by an ellipsoid. This can be done in an affine-invariant way, e.g., by selecting, among all ellipsoids containing the body, the one with the smallest volume; since volume is affine-covariant, this selection is affine-invariant. However, this selection may depend on the choice of the hyperplane. It is therefore desirable to directly approximate the convex cone describing Finsler causality with the quadratic cone, ideally in an affine- invariant way. We prove, however, that on the set of convex cones, there is no affine-covariant characteristic like volume. So, any approximation is necessarily not affine-invariant.
机译:一些物理学家建议,为了更充分地描述时空的因果结构,有必要超越通常的伪黎曼因果关系,而应扩展到更一般的Finsler因果关系。在这种一般情况下,可以受给定事件影响的所有事件的集合在局部上是普通凸锥,而不一定是伪雷曼式二次锥。由于当前所有观察结果都支持伪黎曼因果关系,因此Finsler因果关系锥应接近二次方。因此,期望将一般的凸锥近似为二次锥。如果我们选择一个超平面,并估计圆锥与该超平面的交点,就可以做到这一点。在超平面中,我们需要用椭圆体近似凸体。这可以通过仿射不变的方式来完成,例如,通过在所有包含人体的椭球体中选择体积最小的一个;由于体积是仿射不变的,因此此选择是仿射不变的。但是,该选择可能取决于超平面的选择。因此,理想的是,理想地以仿射不变的方式用二次圆锥直接逼近描述Finsler因果关系的凸圆锥。但是,我们证明,在凸锥集上,没有像体积那样的仿射协变特征。因此,任何近似都不一定是仿射不变的。

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