Page - 389 - in Differential Geometrical Theory of Statistics
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Entropy2016,9, 337
with1Uk thecharacteristic functionof thesetUk. It seemsnatural toextendthedensityobtainedfrom
samples toanotheronebasedonthe trajectories themselvesusinganintegral form:
dk=Ī»ā1 N
ā
i=1 ā« 1
0 1Uk (γi(t))dt (2)
where thenormalizingconstantĪ» is chosensothatdk isadiscreteprobabilitydistribution:
Ī»= P
ā
k=1 N
ā
i=1 ā« 1
0 1Uk (γi(t))dt= N
ā
i=1 ā« 1
0 P
ā
k=1 1Uk (γi(t))dt
andsinceUk,k=1,. . . ,P isapartition:
P
ā
k=1 1Uk (γi(t))=1 (3)
so thatĪ»=N.
Densitycanbeviewedasanempiricalprobabilitydistributionwith theUk consideredasbins
inanhistogram. It is thusnatural toextendtheabovecomputationsoas togiverise toacontinuous
distributiononΩ. For thatpurpose, localweighting techniques, suchaskerneldensityestimation
methods, arewell known in nonparametric statistics, because they are a useful data-drivenway
toyield continuousdensity estimation. Many referencesmaybe found in the literature as in [5,6].
Giventheobservations, theresultingestimationwillbe thesumofweights taking intoaccount the
distancebetweentheobservationsandthelocationxatwhichthedensityhastobeestimated; themore
an observation is close to x, the greater is theweighting. Theweights are deļ¬nedby selecting a
summable functioncenteredontheobservations, calledakernel,usuallydenotedbyK :RāR+ in
theunivariatecase,andasmoothedversionof theParzenāRosenblattdensityestimator [7,8] isused.
Standardchoices for theK functionare theonesusedfornonparametrickernelestimation, like the
Epanechnikovfunction[9]:
K : x ā (
1āx2 )
1[ā1,1](x).
There exists a large variety of kernel functions, and any density function satisfying the
normalizationconditioncanbeconsidered, so that theestimation isaprobabilitydensity.Moreover,
thekernel function isasymmetricpositive function,with theļ¬rstmomentequal tozeroandaļ¬nite
secondordermoment. In themultivariatecase,amultivariatekernel functionK :RqāR+ is selected
that can be expressed bymeans of a real kernelK associatedwith a norm, denoted by ā.ā, inRq
as follows:
K(x)=K(āxā), xāRq.
Thenormalizationconditionbecomes:ā«
Rq K(x)dx= ā«
Rq K(āxā)dx=1.
Akernelversionof thedensity is thendeļ¬nedasamappingd fromĪ© to [0,1]:
d: x ā ā N
i=1 ā«1
0 K(āxāγi(t)ā)dt
āNi=1 ā«
Ī© ā«1
0 K(āxāγi(t)ā)dtdx . (4)
Normalizingthekernel isnotmandatory,as thenormalizationoccurswiththedeļ¬nitionofd. It is
neverthelesseasier toconsider thesekindsofkernels, as isdone innonparametricdensityestimation.
389
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