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Entropy2016,18, 442 m(x)αm′(x)1āˆ’Ī±/m(x) is likely tohaveasmallvariancewhenxvaries insideaslab Ir, especiallywhen α is close to1.Wewill thereforeboundthis ratio termin ∫ Ir m(x)αm′(x)1āˆ’Ī±dx= ∫ Ir m(x) ( m(x)αm′(x)1āˆ’Ī± m(x) ) dx= k āˆ‘ i=1 ∫ Ir wipi(x) ( m′(x) m(x) )1āˆ’Ī± dx. (47) No matter α < 1 or α > 1, the function x1āˆ’Ī± must be monotonic onR+. In each slab Ir, (m′(x)/m(x))1āˆ’Ī± rangesbetweenthese twofunctions:( c′ ν′(r)p ′ ν′(r)(x) cĪ“(r)pĪ“(r)(x) )1āˆ’Ī± and ( c′ Γ′(r)p ′ Γ′(r)(x) cν(r)pν(r)(x) )1āˆ’Ī± , (48) where cν(r)pν(r)(x), cĪ“(r)pĪ“(r)(x), c′ν′(r)p ′ ν′(r)(x)and c ′ Γ′(r)p ′ Γ′(r)(x)aredefinedinEquations (45)and(46). Similar to thedefinitionofAαi,j(I) inEquation(37),wedefine Bαi,j,l(I)= ∫ I wipi(x) ( c′lp ′ l(x) cjpj(x) )1āˆ’Ī± dx. (49) Thereforewehave, Lα(m :m′)=minS, Uα(m :m′)=maxS, S= { āˆ‘ r=1 k āˆ‘ i=1 Bαi,Ī“(r),ν′(r)(Ir), āˆ‘ r=1 k āˆ‘ i=1 Bαi,ν(r),Γ′(r)(Ir) } . (50) Theremainingproblemis toevaluateBαi,j,l(I) inEquation(49). Similar toSection4.1,assuming thecomponentsare in thesameexponential familywithrespect to thenaturalparametersĪø,weget Bαi,j,l(I)=wi c′1āˆ’Ī±l c1āˆ’Ī±j exp ( F(ĪøĀÆ)āˆ’F(Īøi)āˆ’(1āˆ’Ī±)F(θ′l)+(1āˆ’Ī±)F(Īøj) )∫ I p(x; ĪøĀÆ)dx. (51) If ĪøĀÆ= Īøi+(1āˆ’Ī±)θ′lāˆ’(1āˆ’Ī±)Īøj is in thenaturalparameterspace,Bαi,j,l(I)canbecomputedfromthe CDFof p(x; ĪøĀÆ); otherwiseBαi,j,l(I) canbenumerically integrated by its definition inEquation (49). Thecomputationalcomplexity is thesameas thebounds inSection4.2, i.e.,O( (k+k′)). Wehave introducedthreepairsofdeterministic lowerandupperboundsthatenclose the true valueofα-divergencebetweenunivariatemixturemodels. Thus thegapbetweentheupperandlower boundsprovides the additive approximation factor of the bounds. We conclude by emphasizing that the presentedmethodology canbe easily generalized to other divergences [35,40] relying on Hellinger-type integralsHα,β(p : q)= ∫ p(x)αq(x)βdx like theγ-divergence [44]aswell asentropy measures [45]. 5. LowerBoundsof the f-Divergence The f-divergencebetweentwodistributionsm(x)andm′(x) (notnecessarilymixtures) isdefined fora convexgenerator f by: Df(m :m′)= ∫ m(x)f ( m′(x) m(x) ) dx. If f(x)=āˆ’ logx, thenDf(m :m′)=KL(m :m′). 300
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Differential Geometrical Theory of Statistics
Title
Differential Geometrical Theory of Statistics
Authors
FrƩdƩric Barbaresco
Frank Nielsen
Editor
MDPI
Location
Basel
Date
2017
Language
English
License
CC BY-NC-ND 4.0
ISBN
978-3-03842-425-3
Size
17.0 x 24.4 cm
Pages
476
Keywords
Entropy, Coding Theory, Maximum entropy, Information geometry, Computational Information Geometry, Hessian Geometry, Divergence Geometry, Information topology, Cohomology, Shape Space, Statistical physics, Thermodynamics
Categories
Naturwissenschaften Physik
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