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Random Processes in Hyperbolic Spaces Hyperbolic Brownian ...

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3 Tools of Riemannian Geometry<br />

For a proof see, for example, Kühnel (24) Theorem 5.6. Therefore for every tangent vector X(p) ∈<br />

TpM one has<br />

n<br />

X(p) =<br />

i=1<br />

ξ i p ∂i(p), (1.3)<br />

where ξ i p is the directional derivative of the coord<strong>in</strong>ate function x i <strong>in</strong> the direction X(p). For a<br />

function f : M → R, f ∈ C 1 we have<br />

X(p)f =<br />

n<br />

i=1<br />

ξ i p ∂i(p)f.<br />

Def<strong>in</strong>ition 1.1.10. A differentiable vector field X on a n-dimensional manifold M is an association<br />

p ∈ U ⊂ M → X(p) ∈ TpM such that <strong>in</strong> every chart ϕ : U → R n , with coord<strong>in</strong>ates (x 1 , . . . , x n ), the<br />

coefficients ξ i p : U → R <strong>in</strong> the representation (1.3) valid at the each po<strong>in</strong>t p ∈ U are differentiable<br />

functions.<br />

Common notations for the vector field and the directional derivative of a function f : M → R,<br />

f ∈ C 1 <strong>in</strong> the direction of the vector field are<br />

X =<br />

n<br />

ξ i ∂i, Xf =<br />

i=1<br />

n<br />

ξ i ∂if.<br />

The <strong>in</strong>terpretation of X as a derivative operator permits us to consider the iterates of X. If<br />

X and Y are two differentiable vector fields on M and f : M → R, f ∈ C 2 , we can consider the<br />

functions X(Y f) and Y (Xf).<br />

Proposition 1.1.1. Let X and Y be two differentiable vector fields on a C ∞ manifold M. Then<br />

there exists a unique vector filed [X, Y ], which is referred to as the Lie bracket of X and Y , such<br />

that for all f : M → R, f ∈ C 2 ,<br />

i=1<br />

[X, Y ]f = X(Y f) − Y (Xf).<br />

For a proof see, for example, Do Carmo (14) Lemma 5.2.<br />

We <strong>in</strong>troduce now a metric structure on M.<br />

Def<strong>in</strong>ition 1.1.11. An <strong>in</strong>ner product on a vector space V over a field F is a bil<strong>in</strong>ear form<br />

such that is<br />

• symmetric: 〈v, w〉 = 〈w, v〉<br />

• positive def<strong>in</strong>ite: 〈v, v〉 > 0 for all v = 0.<br />

(v, w) ∈ V × V → 〈v, w〉 ∈ F,<br />

Def<strong>in</strong>ition 1.1.12. Given a C ∞ manifold M, def<strong>in</strong>e a Riemannian metric g on M to be a mapp<strong>in</strong>g<br />

that associates with each p ∈ M an <strong>in</strong>ner product<br />

gp : MpT × MpT → R

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