Abstract:A family of probability distributions parametrized by an open domain Λ in R n defines the Fisher information matrix on this domain which is positive semi-definite. In information geometry the standard assumption has been that the Fisher information matrix tensor is positive definite defining in this way a Riemannian metric on Λ. If we replace the "positive definite" assumption by the existence of a suitable torsion-free connection, a foliation with a transversely Hessian structure appears naturally. In the pap… Show more
“…When we deal with the vector tangent bundles the differential operator D ∇∇ * plays many outstanding roles in the global analysis of the base manifold [6]. In general though every vector bundle admits positive metric structures this same claim is far from being true for symplectic structure and for positive signature metric structures.…”
Section: Gauge Structures In a Vector Bundle Ementioning
confidence: 96%
“…We deduce from Corollary 2 that every special statistical manifold supports a canonical (quasi) 4-web, viz 4 foliations in (quasi) general position. Before pursing we remark that among formalisms introduce in [6], many (of them) walk in the category of vector bundles. We go to perform this remark.…”
Section: Proposition 3 ([5])mentioning
confidence: 99%
“…The functor just mentioned is called the general Amari functor of the vector bundle E. According to [6], the general Amari functor yield two restrictions :…”
Section: The Amari Functors In the Category Ga(e)mentioning
confidence: 99%
“…We go to perform a formalism which is developed in [5]. See also [6] for the case of tangent bundles of a manifolds. The concerns are metric structures in vector bundles.…”
Section: Consequently We Go To Encode Every Orbit [∇] = G(e) ⋆ ∇ Withmentioning
confidence: 99%
“…Inspired by the appendix to [4] and by [6] and by we define a map from pairs of gauge structures in the space of differential operators DO(Eo * ⊗ E, T * M ⊗ E * ⊗E). To every pair of gauge structures [(E, ∇), (E, ∇ ⋆ )] we introduce the first order differential operator…”
Section: Gauge Structures In a Vector Bundle Ementioning
Abstract. We deal with finite dimensional differentiable manifolds. All items are concerned with are differentiable as well. The class of differentiability is C ∞ . A metric structure in a vector bundle E is a constant rank symmetric bilinear vector bundle homomorphism of E × E in the trivial bundle line bundle. We address the question whether a given gauge structure in E is metric. That is the main concerns. We use generalized Amari functors of the information geometry for introducing two index functions defined in the moduli space of gauge structures in E. Beside we introduce a differential equation whose analysis allows to link the new index functions just mentioned with the main concerns. We sketch applications in the differential geometry theory of statistics.Reader interested in a former forum on the question whether a giving connection is metric are referred to appendix.
“…When we deal with the vector tangent bundles the differential operator D ∇∇ * plays many outstanding roles in the global analysis of the base manifold [6]. In general though every vector bundle admits positive metric structures this same claim is far from being true for symplectic structure and for positive signature metric structures.…”
Section: Gauge Structures In a Vector Bundle Ementioning
confidence: 96%
“…We deduce from Corollary 2 that every special statistical manifold supports a canonical (quasi) 4-web, viz 4 foliations in (quasi) general position. Before pursing we remark that among formalisms introduce in [6], many (of them) walk in the category of vector bundles. We go to perform this remark.…”
Section: Proposition 3 ([5])mentioning
confidence: 99%
“…The functor just mentioned is called the general Amari functor of the vector bundle E. According to [6], the general Amari functor yield two restrictions :…”
Section: The Amari Functors In the Category Ga(e)mentioning
confidence: 99%
“…We go to perform a formalism which is developed in [5]. See also [6] for the case of tangent bundles of a manifolds. The concerns are metric structures in vector bundles.…”
Section: Consequently We Go To Encode Every Orbit [∇] = G(e) ⋆ ∇ Withmentioning
confidence: 99%
“…Inspired by the appendix to [4] and by [6] and by we define a map from pairs of gauge structures in the space of differential operators DO(Eo * ⊗ E, T * M ⊗ E * ⊗E). To every pair of gauge structures [(E, ∇), (E, ∇ ⋆ )] we introduce the first order differential operator…”
Section: Gauge Structures In a Vector Bundle Ementioning
Abstract. We deal with finite dimensional differentiable manifolds. All items are concerned with are differentiable as well. The class of differentiability is C ∞ . A metric structure in a vector bundle E is a constant rank symmetric bilinear vector bundle homomorphism of E × E in the trivial bundle line bundle. We address the question whether a given gauge structure in E is metric. That is the main concerns. We use generalized Amari functors of the information geometry for introducing two index functions defined in the moduli space of gauge structures in E. Beside we introduce a differential equation whose analysis allows to link the new index functions just mentioned with the main concerns. We sketch applications in the differential geometry theory of statistics.Reader interested in a former forum on the question whether a giving connection is metric are referred to appendix.
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