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Entropy2016,18, 425
parallel transport of thevectorsu1, . . . ,ud of the framealong thedirectionui. A horizontal liftof a
differentiablecurvextâM isacurve inFM tangent toHFM thatprojects toxt.Horizontal liftsare
uniqueupto thechoiceof initial frameu0.
TFM
TâFM
HFMVFM
FMĂgl(n) FM
TMTâM M
h+v â
hh+v
â v
ÏâÏ ÏFM
ÏTM
gFM
gR
Figure3.Relationsbetweenthemanifold, framebundle, thehorizontaldistributionHFM, thevertical
bundle VFM, a Riemannian metric gR, and the sub-Riemannian metric gFM, deïŹned below.
TheconnectionCprovides thesplittingTFM=HFMâVFM. TherestrictionsÏâ|HuM are invertible
mapsHuMâTÏ(u)Mwith inversehu, thehorizontal lift. Correspondingly, theverticalbundleVFM
is isomorphic to the trivialbundleFMĂgl(n). ThemetricgFM :TâFMâTFMhasanimage inthe
subspaceHFM.
2.2.DevelopmentandStochasticDevelopment
Let xt be a differentiable curve on M and ut a horizontal lift. If st is a curve inRd with
components sit suchthat xËt=Hi(u)s i
t,xt is said tobeadevelopmentof st.Correspondingly, st is the
anti-developmentof xt. For each t, thevector st contains framecoordinatesof xËt asdeïŹnedabove.
Similarly, letWtbeanRdvaluedBrownianmotionsothatsamplepathsWt(Ï)âW(Rd).Asolutionto
thestochasticdifferentialequationdUt=âdi=1Hi(Ut)âŠdWit inFM is calledastochasticdevelopment
ofWt inFM. Thesolutionprojects toastochasticdevelopmentXt=Ï(Ut) inM.Wecall theprocess
Wt inRd, that throughÏmapstoXt, thedrivingprocessofXt. LetÏu :W(Rd)âW(M)bethemap
that forïŹxedu sendsapath inRd to itsdevelopmentonM. Its inverseÏâ1u is theanti-development in
RdofpathsonMgivenu.
Equivalent to the fact thatnormaldistributionsN(0,ÎŁ) inRd canbeobtainedas the transition
distributionsofdiffusionprocessesÎŁ1/2Wt stoppedat time t=1,ageneralclassofdistributionson
themanifoldM canbedeïŹnedby stochasticdevelopmentofprocessesWt, resulting inM-valued
randomvariablesX=X1. This familyofdistributionsonM introducedin[2] isdenotedanisotropic
normaldistributions. Thestochasticdevelopmentbyconstructionensures thatUt ishorizontal, andthe
framesare thusparallel transportedalongthestochasticdisplacements. Theeffect is that the frames
staycovariantlyconstant, thusresemblingtheEuclideansituationwhereÎŁ1/2 is spatiallyconstantand
thereforedoesnotchangeasWt evolves. Thus,as furtherdiscussedinSection3.2, thecovariance is
keptconstantateachof the inïŹnitesimalstochasticdisplacements. Theexistenceofasmoothdensity
for the targetprocessXt andsmall timeasymptoticsarediscussed in [3].
Stochastic development gives a map â«
Diff : FM â Prob(M) to the space of probability
distributionsonM. ForeachpointuâFM, themapsendsaBrownianmotion inRd toadistribution
ÎŒubystochasticdevelopmentof theprocessUt inFM, startingatuandlettingÎŒubethedistribution
of X = Ï(U1). The pair (x,u), x = Ï(u) is analogous to the parameters (ÎŒ,ÎŁ) for a Euclidean
normaldistribution: thepointxâM represents thestartingpointof thediffusion,andthe frameu
representsasquarerootÎŁ1/2 of thecovarianceÎŁ. In thegeneralsituationwhereÎŒuhassmoothdensity,
theconstructioncanbeusedtoïŹt theparametersu todatabymaximumlikelihood.Asanexample,
diffusionPCAïŹtsdistributionsobtainedthrough â«
Diff bymaximumlikelihoodtoobservedsamples
inM; i.e., itoptimizes for themost likelyparametersu=(x,u1, . . . ,ud) for theanisotropicdiffusion
process,givingaïŹt to thedataof themanifoldgeneralizationof theEuclideannormaldistribution.
407
Differential Geometrical Theory of Statistics
- Title
- Differential Geometrical Theory of Statistics
- Authors
- Frédéric 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