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Entropy2016,18, 425
parallel transport of thevectorsu1, . . . ,ud of the framealong thedirectionui. A horizontal liftof a
differentiablecurvext∈M isacurve inFM tangent toHFM thatprojects toxt.Horizontal liftsare
uniqueupto thechoiceof initial frameu0.
TFM
T∗FM
HFMVFM
FM×gl(n) FM
TMT∗M M
h+v →
hh+v
→ v
π∗ψ πFM
πTM
gFM
gR
Figure3.Relationsbetweenthemanifold, framebundle, thehorizontaldistributionHFM, thevertical
bundle VFM, a Riemannian metric gR, and the sub-Riemannian metric gFM, defined below.
TheconnectionCprovides thesplittingTFM=HFM⊕VFM. Therestrictionsπ∗|HuM are invertible
mapsHuM→Tπ(u)Mwith inversehu, thehorizontal lift. Correspondingly, theverticalbundleVFM
is isomorphic to the trivialbundleFM×gl(n). ThemetricgFM :T∗FM→TFMhasanimage 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 x˙t=Hi(u)s i
t,xt is said tobeadevelopmentof st.Correspondingly, st is the
anti-developmentof xt. For each t, thevector st contains framecoordinatesof x˙t asdefinedabove.
Similarly, letWtbeanRdvaluedBrownianmotionsothatsamplepathsWt(ω)∈W(Rd).Asolutionto
thestochasticdifferentialequationdUt=∑di=1Hi(Ut)◦dWit inFM is calledastochasticdevelopment
ofWt inFM. Thesolutionprojects toastochasticdevelopmentXt=π(Ut) inM.Wecall theprocess
Wt inRd, that throughϕmapstoXt, thedrivingprocessofXt. Letϕu :W(Rd)→W(M)bethemap
that forfixedu sendsapath inRd to itsdevelopmentonM. Its inverseϕ−1u is theanti-development in
RdofpathsonMgivenu.
Equivalent to the fact thatnormaldistributionsN(0,Σ) inRd canbeobtainedas the transition
distributionsofdiffusionprocessesΣ1/2Wt stoppedat time t=1,ageneralclassofdistributionson
themanifoldM canbedefinedby 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, thusresemblingtheEuclideansituationwhereΣ1/2 is spatiallyconstantand
thereforedoesnotchangeasWt evolves. Thus,as furtherdiscussedinSection3.2, thecovariance is
keptconstantateachof the infinitesimalstochasticdisplacements. Theexistenceofasmoothdensity
for the targetprocessXt andsmall timeasymptoticsarediscussed in [3].
Stochastic development gives a map ∫
Diff : FM → Prob(M) to the space of probability
distributionsonM. Foreachpointu∈FM, themapsendsaBrownianmotion inRd toadistribution
μubystochasticdevelopmentof theprocessUt inFM, startingatuandlettingμubethedistribution
of X = π(U1). The pair (x,u), x = π(u) is analogous to the parameters (μ,Σ) for a Euclidean
normaldistribution: thepointx∈M represents thestartingpointof thediffusion,andthe frameu
representsasquarerootΣ1/2 of thecovarianceΣ. In thegeneralsituationwhereμuhassmoothdensity,
theconstructioncanbeusedtofit theparametersu todatabymaximumlikelihood.Asanexample,
diffusionPCAfitsdistributionsobtainedthrough ∫
Diff bymaximumlikelihoodtoobservedsamples
inM; i.e., itoptimizes for themost likelyparametersu=(x,u1, . . . ,ud) for theanisotropicdiffusion
process,givingafit to thedataof themanifoldgeneralizationof theEuclideannormaldistribution.
407
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
- Kategorien
- Naturwissenschaften Physik