On the definition and examples of cones and Finsler spacetimes

A systematic study of (smooth, strong) cone structures C and Lorentz–Finsler metrics L is carried out. As a link between both notions, cone triples ( Ω , T , F ) , where Ω (resp. T ) is a 1-form (resp. vector field) with Ω ( T ) ≡ 1 and F , a Finsler metric on ker ( Ω ) , are introduced. Explicit de...

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Bibliographic Details
Published inRevista de la Real Academia de Ciencias Exactas, Físicas y Naturales. Serie A, Matemáticas Vol. 114; no. 1
Main Authors Javaloyes, Miguel Angel, Sánchez, Miguel
Format Journal Article
LanguageEnglish
Published Cham Springer International Publishing 2020
Springer Nature B.V
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Summary:A systematic study of (smooth, strong) cone structures C and Lorentz–Finsler metrics L is carried out. As a link between both notions, cone triples ( Ω , T , F ) , where Ω (resp. T ) is a 1-form (resp. vector field) with Ω ( T ) ≡ 1 and F , a Finsler metric on ker ( Ω ) , are introduced. Explicit descriptions of all the Finsler spacetimes are given, paying special attention to stationary and static ones, as well as to issues related to differentiability. In particular, cone structures C are bijectively associated with classes of anisotropically conformal metrics L , and the notion of cone geodesic is introduced consistently with both structures. As a non-relativistic application, the time-dependent Zermelo navigation problem is posed rigorously, and its general solution is provided.
ISSN:1578-7303
1579-1505
DOI:10.1007/s13398-019-00736-y