2018
DOI: 10.5486/pmd.2018.8126
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The cut locus of a Randers rotational 2-sphere of revolution

Abstract: In the present paper we study structure of the cut locus of a Randers rotational 2-sphere of revolution (M, F = α + β). We show that in the case when Gaussian curvature of the Randers surface is monotone along a meridian the cut locus of a point q ∈ M is a point on a subarc of the opposite half bending meridian or of the antipodal parallel (Theorem 1.1). More generally, when the Gaussian curvature is not monotone along the meridian, but the cut locus of a point q on the equator is a subarc of the same equator,… Show more

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Cited by 10 publications
(10 citation statements)
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“…since along the extremal the Hamiltonian is constant and equal to −p 0 . Putting (23) in (22), one has…”
Section: Micro-local Analysis Of the Extremal Solutionsmentioning
confidence: 99%
See 1 more Smart Citation
“…since along the extremal the Hamiltonian is constant and equal to −p 0 . Putting (23) in (22), one has…”
Section: Micro-local Analysis Of the Extremal Solutionsmentioning
confidence: 99%
“…Parallel development were obtained in the frame of space navigation where geometric analysis is combined with numerical methods, see again [11] for a general reference for such contributions. In the frame of Zermelo navigation problem with a small current, called Randers metrics, some results were obtained recently for sphere of revolutions [22].…”
Section: Introductionmentioning
confidence: 99%
“…Note that in (2), the current is along the parallels only, which is sufficient to cover the two founding examples. We refer to [11] for a case study in the differential geometric frame, in the case of a weak current, that is Randers problems in Finsler geometry [2], assuming F 0 g < 1.…”
Section: Introductionmentioning
confidence: 99%
“…We will focus on Finsler metrics of Randers type obtained as solutions of the Zermelo's navigation problem, for the navigation data (M, h), where h is the canonical Riemannian metric on the topological cylinder h = dr 2 + m 2 (r)dθ 2 , and W = A(r) ∂ ∂r + B ∂ ∂θ is a vector field on M. Observe that our wind is more general than a Killing vector field, hence our theory presented here is a generalization of the classical study of geodesics and cut locus for Randers metrics obtained as solutions of the Zermelo's navigation problem with Killing vector fields studied in [10,11] (see also [12] for another attempt to generalize the Zermelo's navigation problem). Nevertheless, by taking the wind W in this way, we obtain a quite general Randers metric on M which is a Finsler metric of revolution and whose geodesics and cut locus can be computed explicitly.…”
Section: Introductionmentioning
confidence: 95%