Continuous Wavelet Transform on the Hyperboloid - Université de ...

Continuous Wavelet Transform on the Hyperboloid - Université de ... Continuous Wavelet Transform on the Hyperboloid - Université de ...

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a=0.5, χ=0, φ=0 a=1, χ=0, φ=0 1.6 1.4 1.2 1 0.8 0.6 0.4 0.2 0 −0.2 1 0.8 0.7 0.6 0.5 0.4 0.3 0.2 0.1 0 −0.1 1 0.5 1 0.5 1 0 0.5 0 0.5 −0.5 −0.5 0 −0.5 −0.5 0 −1 −1 −1 −1 a=0.5, χ=1, φ=π/2 a=0.5, χ=1, φ=3π/4 1.6 1.4 1.2 1 0.8 0.6 0.4 0.2 0 −0.2 1 1.6 1.4 1.2 1 0.8 0.6 0.4 0.2 0 −0.2 1 0.5 1 0.5 1 0 0.5 0 0.5 −0.5 −0.5 0 −0.5 −0.5 0 −1 −1 −1 −1 a=0.5, χ=0.75, φ=π a=0.5, χ=2.75, φ=π 1.6 1.4 1.2 1 0.8 0.6 0.4 0.2 0 −0.2 1 1.6 1.4 1.2 1 0.8 0.6 0.4 0.2 0 −0.2 1 0.5 1 0.5 1 0 0.5 0 0.5 −0.5 −0.5 0 −0.5 −0.5 0 −1 −1 −1 −1 Fig. 10. The hyperbolic DOG wavelet fψ ϑ ,forϑ = 2 at different scales a and positions (χ, ϕ), viewed on the unit disk in 3-D perspective. any ρ [Alonso et al., 2002]: ( ) − 1 E ρ ν,ξ (x) = x0 2 − ˆn⃗x −iνρ , (83) ρ for x ∈ H 2 +ρ , (x2 = ρ 2 ). The Inönü-Wigner contraction limit of the Lorentz to the Euclidean group SO(2, 1) + → ISO(2) + is the limit at ρ →∞for (83) 26

Fig. 11. The hyperbolic DOG wavelet fψ ϑ in the disk, for ϑ = 2 at different scales a and positions (χ, ϕ). with x 0 ≈ ρ, ⃗x 2 ≪ ρ 2 , i.e 27

Fig. 11. The hyperbolic DOG wavelet fψ ϑ in <strong>the</strong> disk, for ϑ = 2 at different scales a<br />

and positi<strong>on</strong>s (χ, ϕ).<br />

with x 0 ≈ ρ, ⃗x 2 ≪ ρ 2 , i.e<br />

27

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