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It is not the case that The Finsler metric field F_p(dx) must be a Riemannian metric field of some signature
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Reasons For
2 perspectives
Reason for 1 of 2
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1.
Finsler geometry admits non-Riemannian metrics (e.g., Berwald, Randers types) that yield unique, torsion-free connections without reducing to Riemannian structure.
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2.
The Chern connection in Finsler geometry is symmetric and linear yet operates on the pulled-back bundle, not the tangent bundle, undermining Weyl's uniqueness inference.
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Reason for 2 of 2
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1.
Weyl's Postulate of Freedom is satisfied by anisotropic Finsler structures where the metric depends on direction, not merely position, violating the isotropy Riemannian signature requires.
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2.
Élie Cartan demonstrated in 1934 that the axiom of free mobility—the precise formal content of Weyl's postulate—is insufficient to exclude non-quadratic Finsler norms from physical geometry.
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Reasons Against
1 perspective
Reason against
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1.
The geometry satisfies the Postulate of Freedom (the nature of space imposes no restrictions on admissible metrical relations)
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2.
The geometry determines a unique, symmetric, linear connection Γ
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