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Discrete Holomorphic Local Dynamical Systems

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Uniformisation of Foliations by Curves 155<br />

and meromorphic maps<br />

πF : VF ��� X, ΠF : UF ��� X<br />

such that, for any transversal T ⊂ X 0 , we have Q −1<br />

F (T )=VT , qF |T = qT ,<br />

πF | Q −1<br />

F (T ) = πT ,etc.<br />

Remark that if D ⊂ X 0 is a small disc contained in some leaf Lp of F , p ∈ D,<br />

then Q −1<br />

F (D) is naturally isomorphic to the product �Lp × D: foreveryq ∈ D, �Lq is<br />

the same as �Lp, but with a different basepoint. More precisely, thinking to points<br />

of �Lq as equivalence classes of paths starting at q, we see that for every q ∈ D<br />

the isomorphism between �Lq and �Lp is completely canonical, once D is fixed and<br />

because D is contractible. This means that D can be lifted, in a canonical way, to a<br />

(D), transverse to the fibers. In this way, by varying D in<br />

foliation by discs in Q −1<br />

F<br />

X 0 , we get in the full space VF a nonsingular foliation by curves � F , which projects<br />

by QF to F 0 .<br />

If γ : [0,1] → X 0 is a loop in a leaf, γ(0)=γ(1)=p, then this foliation � F permits<br />

to define a monodromy map of the fiber �Lp into itself. This monodromy map is just<br />

the covering transformation of �Lp corresponding to γ (which may be trivial, if the<br />

holonomy of the foliation along γ is trivial).<br />

In a similar way, in the space UF we get a canonically defined nonsingular foliation<br />

by curves � F , which projects by PF to F 0 . And we have a fiberwise covering<br />

FF : UF → VF<br />

which is a local diffeomorphism, sending � F to � F .<br />

γ = q<br />

q F (X 0 )<br />

γ from q to p<br />

V F<br />

L q<br />

L p<br />

γ = p<br />

F<br />

(over a leaf)<br />

In the spaces UF and VF we also have the graphs of the sections pF and qF .<br />

They are not invariant by the foliations � F and � F : in the notation above, with D<br />

in a leaf and p,q ∈ D, the basepoint qF (q) ∈ �Lq corresponds to the constant path<br />

γ(t) ≡ q, whereas the point of �Lq in the same leaf (of � F )ofqF (p) ∈ �Lp corresponds

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