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Differential Geometrical Theory of Statistics
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Entropy2016,18, 277 Conclusion1. UsingPropositions4and1, ifΦ=[η,1−η]× [μmin,μmax]2, the sequence (Dˆϕ(pφk,pφT))k defined throughFormula (2) convergesand there exists a subsequence (φN(k))whichconverges toa stationary pointof the estimateddivergence.Moreover, every limitpointof the sequence (φk)k is a stationarypointof the estimateddivergence. Ifwe are using the kernel-baseddual estimator given by (3)with aGaussian kernel density estimator, thenfunctionφ → Dˆϕ(pφ,pφT) is continuouslydifferentiableoverΦevenif themeansμ1 andμ2 arenotbounded. Forexample, takeϕ=ϕγ definedby(1). There isoneconditionwhichrelates thewindowof thekernel, sayw,with thevalueofγ. Indeed,usingFormula (3),wecanwrite Dˆϕ(pφ,pφT)= 1 γ−1 ∫ pγφ Kγ−1n,w (y)dy− 1 γn n ∑ i=1 pγφ Kγn,w (yi)− 1γ(γ−1). Inorder tostudythecontinuityandthedifferentiabilityof theestimateddivergencewithrespect toφ, it suffices tostudythe integral term.Wehave pγφ Kγ−1n,w (y)= ( λ√ 2π exp [ −12(y−μ1)2 ] + 1−λ√ 2π exp [ −12(y−μ2)2 ])γ ( 1 nw∑ n i=1exp [ −(y−yi)22w2 ])γ−1 . The dominating term at infinity in the nominator is exp(−γy2/2), whereas it is exp(−(γ−1)y2/(2w2)) in thedenominator. It sufficesnowinorder that the integrandtobebounded byan integrable function independentlyofφ= (λ,μ) thatwehave−γ+(γ−1)/w2< 0. That is −γw2+γ−1<0,which isequivalent toγ(w2−1)<−1. Thisargumentalsoholds ifwedifferentiate the integrandwithrespect toλoreitherof themeansμ1 orμ2. Forγ=2(thePearson’sχ2),weneed w2>1/2. Forγ=1/2(theHellinger), there isnoconditiononw. ClosednessofΦ0 isprovedsimilarlytothepreviouscase. Boundedness,however,mustbetreated differentlysinceΦ isnotnecessarilycompactandis supposedtobeΦ=[η,1−η]×R2. Forsimplicity, takeϕ=ϕγ. The idea is tochooseφ0 an initializationfor theproximalalgorithminawaythatΦ0does not includeunboundedvaluesof themeans. Continuityofφ → Dˆϕ(pφ,pφT)permits calculationof the limitswheneither (orboth)of themeans tends to infinity. Ifboth themeansgoto infinity, then pφ(x)→0,∀x. Thus, forγ∈ (0,∞)\{1},wehave Dˆϕ(pφ,pφT)→ 1γ(γ−1). Forγ<0, the limit is infinity. Ifonlyoneof themeans tends to∞, thenthecorrespondingcomponentvanishes fromthemixture. Thus, ifwechooseφ0 suchthat: Dˆϕ(pφ0,pφT) < min ( 1 γ(γ−1),infλ,μDˆϕ(p(λ,∞,μ),pφT) ) ifγ∈ (0,∞)\{1}, (18) Dˆϕ(pφ0,pφT) < inf λ,μ Dˆϕ(p(λ,∞,μ),pφT) ifγ<0, (19) thenthealgorithmstartsatapointofΦwhosefunctionvalue is inferior to the limitsof Dˆϕ(pφ,pφT) at infinity. ByProposition 1, the algorithmwill continue todecrease thevalue of Dˆϕ(pφ,pφT) and nevergoesback to the limitsat infinity. Inaddition, thedefinitionofΦ0 permits toconclude that if φ0 is chosenaccording toconditions (18)and(19), thenΦ0 isbounded. Thus,Φ0 becomescompact. Unfortunately thevalueof infλ,μ Dˆϕ(p(λ,∞,μ),pφT)canbecalculatedbutnumerically.Wewill seenext that in thecaseof the likelihoodfunction,asimilarconditionwillbe imposedfor thecompactnessof Φ0, andtherewillbenoneedforanynumerical calculus. Conclusion 2. UsingPropositions 4 and 1, under conditions (18) and (19) the sequence (Dˆϕ(pφk,pφT))k defined throughFormula (3) converges and there exists a subsequence (φN(k)) that converges to a stationary 264
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Differential Geometrical Theory of Statistics
Titel
Differential Geometrical Theory of Statistics
Autoren
Frédéric 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
Schlagwörter
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