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

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4<br />

p=0.5<br />

4<br />

p=1<br />

3.5<br />

3.5<br />

3<br />

3<br />

2.5<br />

2.5<br />

2<br />

2<br />

1.5<br />

1.5<br />

1<br />

1<br />

0.5<br />

0.5<br />

0<br />

−4 −3 −2 −1 0 1 2 3 4<br />

0<br />

−4 −3 −2 −1 0 1 2 3 4<br />

Fig. 4. Cross-secti<strong>on</strong> of c<strong>on</strong>ic projecti<strong>on</strong>s for different values of parameter p.<br />

x<br />

0<br />

H 2 +<br />

a<br />

P<br />

P a<br />

N<br />

P<br />

P<br />

x<br />

1<br />

C<br />

0<br />

P<br />

P<br />

Pa<br />

P<br />

0<br />

x<br />

2<br />

Fig. 5. Acti<strong>on</strong> of a dilati<strong>on</strong> a <strong>on</strong> <strong>the</strong> hyperboloid H 2 + by c<strong>on</strong>ic projecti<strong>on</strong> with<br />

parameter p =1.<br />

The acti<strong>on</strong> of dilati<strong>on</strong> by c<strong>on</strong>ic projecti<strong>on</strong> is given by<br />

sinh pχ a = a sinh pχ (21)<br />

The particular case p = 1 is <strong>de</strong>picted in Figure 5. The dilated point x a ∈ H+<br />

2<br />

is<br />

x a =(coshχ a , sinh χ a cos ϕ, sinh χ a sin ϕ), (22)<br />

with polar coordinates θ a =(χ a ,ϕ). The behaviour of dist(x N , x a ), with x N<br />

being <strong>the</strong> North Pole, is shown in Figure 6 in <strong>the</strong> case p =0.1, p =0.5 and<br />

p = 1. We can see that this is an increasing functi<strong>on</strong> with respect to <strong>the</strong><br />

dilati<strong>on</strong> a.<br />

It is also interesting to compute <strong>the</strong> acti<strong>on</strong> of dilati<strong>on</strong>s in <strong>the</strong> boun<strong>de</strong>d versi<strong>on</strong><br />

of H+ 2 . The latter is obtained by applying <strong>the</strong> stereographic projecti<strong>on</strong> from<br />

<strong>the</strong> South Pole of H 2 and it maps <strong>the</strong> upper sheet H+ 2 <strong>on</strong>to <strong>the</strong> open unit disc<br />

9

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