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Entropy2016,18, 433
Wehave introducedthedoublecomplex{
C : Cij=Ciτ(A∗,A∗)⊗Cjτ(A,C∞(M)), δij }
.
It gives rise to spectral sequenceswhichmaybeuseful for computing theKVcohomologies
H∗τ (A∗,A∗) andH∗KV (A,C∞(M)). That is not thepurposeof thispaper. However thisdouble
complex isuseful for replacingthefirstorderdifferentialequation
D∇∇ ∗
(ψ)=0
bythehomologicalequation
δ1,2qψ=0.
WehaveprovedthehomologicalnatureofthespaceofgaugehomomorphismsM(∇,∇∗). This is
useful for relatingthe imageofM(∇,∇∗) inH1τ(A∗,A∗)andthepairH2dR(M),H1,2(C).
8.B.TheTheoryofStatisticaLModels
In the introductionof thispaperwehaverecalledtheproblemraisedbyPeterMcCullagh.
What isastatisticalmodel [30]?
Bythewaywehaverecalledavariant requestofMishaGromov.
InaSearchforaStructure. TheFisher Information[15,16].
McCullaghandGromovchoose thesameframeworkforaddressingtheirpurpose,The theoryof
category. ThisPartB isdevotedto thesamepurpose.
Further themoduli space of isomorphism class of objects of a category C is denoted by [Ca].
Ingeneral it isdifficult tofindan invariant invawhichencodes [Ca]. Subsequently to thequestions
raisedbyMcCullaghandbyGromov themoduli spaceof isomorphismclass of statisticalmodels
is discussed in this Part B.Nowadays, there exists awell established theory of statisticalmodels.
The classical references are Amari [17], Amari and Nagaoka [18]. Other remarkable references
are Barndorff-Nielsen (Indian Journal ofMathematics 29, RamanujanCentenaryVolume) [21,24],
KassandVos[37],Murray-Rice (Chapter1,Section15 in[22]). InPartAof thispaperwehavebeen
dealingwith thiscurrent theory. Ithasbeencalled the local theory.Wesuggest readingtheattemptby
McCullaghtoestablishaconceptuallyconsistent theoryofstatisticalmodels [30]. In its time, thepaper
ofMcCullaghhadbeentheobjectofcontroversyandquestions.
Weareaimedatre-establishingthe theoryofstatisticalmodels.Ourmotivationshaveemerged
fromsomecriticisms.
The current theory presents somedeficiencies thatweplan outlining. (i) Aweakness of the
current theory is its lacking in geometry; (ii) In the literature on the information geometrymany
referencesdefine anm-dimensional statisticalmodel as anopen subset of anEuclidean spaceRm.
Though thisdefinitionmaybeuseful fordealingwithcoordinate functions, it is topologicallyand
geometricallyuseless. LetΓbe thegroupofmeasurable isomorphismsof ameasurable set (Ξ,Ω).
The informationgeometryof a statisticalmodelM includes thegeometry in the senseofErlangen
programof thepair [M,Γ].
Let M and M∗ be m-dimensional statistical models for the same measurable set (Ξ,Ω).
An isomorphismofM onM∗ looks like an sufficient statistic. The geometries [M,Γ] and [M∗,Γ]
provide thesameinformation. So the impacton theapplied informationgeometryof the theoryof
moduli space isnotable. Subsequently thesearch for characteristic invariantspresentsa challenge.
An invariant is calledcharacteristic if itdetermineamodelup to isomorphism. Soacharacteristic
invariant encodes themoduli space. That increases the interest in the search of bothMcCullagh
andGromov.
The Fisher information ofwidely usedmodels areHessianmetrics [52]. This observation is
relevant.However theFisher information isnotacharacteristic invariant.
199
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