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RANDOM FIELDS AND THEIR GEOMETRY

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18 1. Random fields<br />

independent of t. We call such a measure ν left relatively invariant under<br />

G. It is easy to see that D(g) is a C ∞ homomorphism from G into the<br />

multiplicative group of positive real numbers, i.e. D(g1g2) = D(g1)D(g2).<br />

We say that ν is left invariant with respect to G if, and only if, it is left<br />

relatively-invariant and D ≡ 1.<br />

Here, finally, is the result.<br />

Lemma 1.4.2 Suppose G acts smoothly on a smooth manifold T and ν<br />

is left relatively invariant under G. Let D be as in (1.4.15) and let W be<br />

Gaussian ν-noise on T . Then, for any F ∈ L 2 (T, ν),<br />

f(g) =<br />

1<br />

� D(g) W (F ◦ θ g −1),<br />

is a left stationary Gaussian random field on G.<br />

Proof. We must prove that<br />

E {f(g1)f(g2)} = C(g −1<br />

1 g2)<br />

for some C : G → R. From the definition of W , we have,<br />

E {f(g1)f(g2)} =<br />

�<br />

1<br />

� � � �<br />

� F θ −1<br />

g (t) F θ −1<br />

1<br />

g (t) ν(dt)<br />

2<br />

D(g1)D(g2) T<br />

� �<br />

�<br />

=<br />

F (θg2(t)) F (t) θg2∗(ν)(dt)<br />

=<br />

=<br />

1<br />

� D(g1)D(g2)<br />

D(g2)<br />

� D(g1)D(g2)<br />

�<br />

T<br />

T<br />

�<br />

D(g −1<br />

1 g2)<br />

�<br />

F<br />

M<br />

∆<br />

= C(g −1<br />

1 g2)<br />

F<br />

θ g −1<br />

1<br />

�<br />

θ −1<br />

g1 g2(t)<br />

�<br />

F (t) ν(dt)<br />

�<br />

θ g −1<br />

1 g2(t)<br />

�<br />

F (t) ν(dt)<br />

This completes the proof. ✷<br />

It is easy to find simple examples to which Lemma 1.4.2 applies. The most<br />

natural generic example of a Lie group acting on a manifold is its action on<br />

itself. In particular, any right Haar measure is left relatively-invariant, and<br />

this is a way to generate stationary processes. To apply Lemma 1.4.2 in<br />

this setting one needs only to start with a Gaussian noise based on a Haar<br />

measure on G. In fact, this is the example (1.4.12) with which we started<br />

this Section.<br />

A richer but still concrete example of a group G acting on a manifold T<br />

is given by G = GL(N, R) × R N acting 19 on T = R N . For g = (A, t) and<br />

19 Recall that GL(N, R) is the (general linear) group of transformations of R N by<br />

rotation.

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