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Differential Geometrical Theory of Statistics
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Entropy2017,19, 7 Theorem 2 (cf. [10,24]). For a q-exponential family Sq, two statistical manifolds (Sq,gF,∇(2q−1)) and (Sq,g,∇q(e))are1-conformally equivalent. Inparticular, an invariant statisticalmanifold (Sq,gF,∇(2q−1)) is 1-conformallyflat. Riemannianmetrics andcubic formshave the followingrelations: gqij(θ) = q Zq(p) gFij(θ), (16) Cqijk(θ) = q Zq(p) (2q−1)CFijk(θ) − q Zq(p) { gFij∂k lnZq(p)+g F jk(θ)∂i lnZq(p)+g F ki(θ)∂j lnZq(p) } . (17) Proof. The results were essentially obtained in [10]. However, we give a simpler proof for Equations (16)and(17).Thekeyideaisasequenceofescortdistributionsandtheescortrepresentations ofgF andCF inTheorem1. FromEquation(10),wedirectlyobtain theconformalequivalencerelation(16)usingtheescort representationofgF in (12). Bydifferentiating(9)andtakinganintegration,weobtain 0 = ∫ Ω u′′ ( ∑θlFl(x)−ψ(θ) ) (Fi(x)−∂iψ(θ))(Fj(x)−∂jψ(θ))(Fk(x)−∂kψ(θ))dx − ∫ Ω u′ ( ∑θlFl(x)−ψ(θ) ) (Fk(x)−∂kψ(θ))∂i∂jψ(θ)dx − ∫ Ω u′ ( ∑θlFl(x)−ψ(θ) ) (Fi(x)−∂iψ(θ))∂j∂kψ(θ)dx − ∫ Ω u′ ( ∑θlFl(x)−ψ(θ) ) (Fj(x)−∂jψ(θ))∂k∂iψ(θ)dx − ∫ Ω u ( ∑θlFl(x)−ψ(θ) ) ∂i∂j∂kψ(θ)dx. SinceZq(p)= ∫ ΩPq(x;θ)dx,wehave ∂iZq(p)= ∂i ∫ Ω Pq(x;θ)dx= ∫ Ω ∂iPq(x;θ)dx= ∫ Ω P˜q(x;θ)(Fi(x)−∂iψ(θ))dx. Fromtheescort representationofCF in (13), andProposition1,weobtainEquation (17) since gqij(θ)= ∂i∂jψ(θ)andC q ijk(θ)= ∂i∂j∂kψ(θ). Weremarkthat thecubic formof (Sq,gF,∇(2q−1)) isnotCF but (2q−1)CF. The difference of a α-divergence and a q-relative entropy is only the normalization q/Zq(p). This implies thatanormalizationforprobabilitydensity imposesageneralizedconformalchangefora statisticalmodel. In thenextpartof this section, letusconsideranotherstatisticalmanifoldonSq (cf. [6,17,26]). Recall thataFishermetricgF has the followingrepresentation: gFij(θ)= ∫ Ω (∂i lnpθ)(∂jpθ)dx. In information geometry, ∂i lnpθ is called an e-representation (exponential representation) of pθ, and∂jpθ is calledam-representation (mixture representation). Intuitively,∂i lnpθ and∂jpθ areregarded as tangentvectorsonastatisticalmodel.HenceaFishermetric is regardedasaL2-innerproductof e- andm-representations. Letusgeneralize e-andm-representations foraq-exponential family. For pθ ∈Sq,wecall∂i lnq pθ aq-score function. ThenwedefineaRiemannianmetricgM by gMij (θ)= ∫ Ω (∂i lnq pθ)(∂jpθ)dx. (18) 320
zurĂźck zum  Buch Differential Geometrical Theory of Statistics"
Differential Geometrical Theory of Statistics
Titel
Differential Geometrical Theory of Statistics
Autoren
FrĂŠdĂŠric Barbaresco
Frank Nielsen
Herausgeber
MDPI
Ort
Basel
Datum
2017
Sprache
englisch
Lizenz
CC BY-NC-ND 4.0
ISBN
978-3-03842-425-3
Abmessungen
17.0 x 24.4 cm
Seiten
476
SchlagwĂśrter
Entropy, Coding Theory, Maximum entropy, Information geometry, Computational Information Geometry, Hessian Geometry, Divergence Geometry, Information topology, Cohomology, Shape Space, Statistical physics, Thermodynamics
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Differential Geometrical Theory of Statistics