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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Published in | Revista de la Real Academia de Ciencias Exactas, Físicas y Naturales. Serie A, Matemáticas Vol. 114; no. 1 |
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Main Authors | , |
Format | Journal Article |
Language | English |
Published |
Cham
Springer International Publishing
2020
Springer Nature B.V |
Subjects | |
Online Access | Get full text |
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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. |
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ISSN: | 1578-7303 1579-1505 |
DOI: | 10.1007/s13398-019-00736-y |