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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 (Îłi(t))dt (2) where thenormalizingconstantλ is chosensothatdk isadiscreteprobabilitydistribution: λ= P ∑ k=1 N ∑ i=1 ∫ 1 0 1Uk (Îłi(t))dt= N ∑ i=1 ∫ 1 0 P ∑ k=1 1Uk (Îłi(t))dt andsinceUk,k=1,. . . ,P isapartition: P ∑ k=1 1Uk (Îłi(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 deïŹnedby 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 theïŹrstmomentequal tozeroandaïŹnite 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 thendeïŹnedasamappingd 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 thenormalizationoccurswiththedeïŹnitionofd. It is neverthelesseasier toconsider thesekindsofkernels, as isdone innonparametricdensityestimation. 389
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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
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Differential Geometrical Theory of Statistics