Seite - 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=λ−1 N
∑
i=1 ∫ 1
0 1Uk (γi(t))dt (2)
where thenormalizingconstantλ is chosensothatdk isadiscreteprobabilitydistribution:
λ= P
∑
k=1 N
∑
i=1 ∫ 1
0 1Uk (γi(t))dt= N
∑
i=1 ∫ 1
0 P
∑
k=1 1Uk (γi(t))dt
andsinceUk,k=1,. . . ,P isapartition:
P
∑
k=1 1Uk (γi(t))=1 (3)
so thatλ=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 definedby selecting a
summable functioncenteredontheobservations, calledakernel,usuallydenotedbyK :R→R+ in
theunivariatecase,andasmoothedversionof theParzen–Rosenblattdensityestimator [7,8] isused.
Standardchoices for theK functionare theonesusedfornonparametrickernelestimation, like the
Epanechnikovfunction[9]:
K : x → (
1−x2 )
1[−1,1](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 thefirstmomentequal tozeroandafinite
secondordermoment. In themultivariatecase,amultivariatekernel functionK :Rq→R+ is selected
that can be expressed bymeans of a real kernelK associatedwith a norm, denoted by ‖.‖, inRq
as follows:
K(x)=K(‖x‖), x∈Rq.
Thenormalizationconditionbecomes:∫
Rq K(x)dx= ∫
Rq K(‖x‖)dx=1.
Akernelversionof thedensity is thendefinedasamappingd fromΩ to [0,1]:
d: x → ∑ N
i=1 ∫1
0 K(‖x−γi(t)‖)dt
∑Ni=1 ∫
Ω ∫1
0 K(‖x−γi(t)‖)dtdx . (4)
Normalizingthekernel isnotmandatory,as thenormalizationoccurswiththedefinitionofd. It is
neverthelesseasier toconsider thesekindsofkernels, as isdone innonparametricdensityestimation.
389
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