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Entropy2016,18, 98
(ii)Notethefollowingeasyinequalities |r1−r2|≤ |r1|+ |r2|≤ √ 2|r|,whichyieldsinh( |r1−r2|2 )≤
1
2e |r|√
2 . This last inequalityshowsthatζ2(σ) isfinite forallσ< √
2. Inorder tocheckζ2( √
2)=∞, it is
necessary toshow: ∫
R2 exp(−|r|√
2 + |r1−r2|
2 )dr1dr2=∞ (40)
The last integral is,uptoaconstant,greater than ∫
Cexp (
−|r|+ |r1−r2|√
2 )
dr1dr2,where:
C={(r1,r2)∈R2 : r1≥−r2,r2≤0}={(r1,r2)∈R2 : r1≥|r2|,r2≤0}.
OnC,
−|r|+ |r1−r2|√
2 =−|r|+ r1−r2√
2 ≥− √
2r1+ r1−r2√
2 = −r1−r2√
2
However, ∫
Cexp (−r1−r2√
2 )
dr1dr2=∞by integratingwithrespect to r1 andthen r2,whichshows
Equation(40).
D.TheLawofX inAlgorithm1
As stated in Appendix A, the uniform distribution on O(m) is given by 1
ω′m det(θ), where
ω′m= 2 mπm 2/2
Γm(m/2) . LetY(s,V) =V†diag(es1, · · · ,esm)V,with s= (s1, · · · ,sm). SinceX =Y(r,U), for
anytest functionϕ :Pm→R,
E[ϕ(X)]= 1
ω′m ∫
O(m)×Rm ϕ(Y(s,V))p(s)det(θ) m
∏
i=1 dsi (41)
Here, det(θ) = ∧
i<j θij and θij = ∑kVjkdVik. On the other hand, by Proposition
4,∫
Pm ϕ(Y)p(Y| I,σ)dv(Y)canbeexpressedas:
(m!2m)−1 × 8m(m−1)4 1
ζm(σ) ∫
O(m) ∫
Rm ϕ(Y(s,V))e− |s|
σ det(θ)∏
i<j sinh (|si−sj|
2 ) m
∏
i=1 dsi
whichcoincideswithEquation(41).
References
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381
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