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Discrete Holomorphic Local Dynamical Systems

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76 Eric Bedford<br />

Fig. 4 Slice W u (q β ) ∩ K +<br />

Problem Suppose that J is connected, and f is hyperbolic. How do you write J as a<br />

quotient of the solenoid? What quotients can appear?<br />

Notes. The geometry of U + is discussed further in [HO]. The problem of writing<br />

J as a quotient of the solenoid is discussed in [BS7]. The thesis of Oliva [O] gives<br />

a number of computer experiments that are helpful in understanding what identifications<br />

can appear when writing J as a quotient. The papers [I] and [IS] give a<br />

combinatorial/topological approach to this problem.<br />

1.7 Currents on R N<br />

Let D k be the set of smooth k-forms on RN with compact support. We define the<br />

space of k-currents to be the dual: D ′ k :=(Dk ) ′ . A basic example is the current of integration.LetM⊂<br />

RN be a k-dimensional submanifold which is oriented and has locally<br />

bounded (k-dimensional) area. Then the current of integration [M] is defined by<br />

D k �<br />

∋ ϕ ↦→〈[M],ϕ〉 = ϕ.<br />

If ϕ is a k-form, and if t is a k-vector, then x ↦→ ϕ(x)·t is a scalar-valued function.<br />

Now let ν be a Borel measure on RN ,andlett(x) denote a field of k-vectors on RN which is Borel measurable, and which is locally integrable with respect to ν. Then<br />

the current T = tν is defined by the action<br />

D k �<br />

∋ ϕ ↦→〈T,ϕ〉 := ϕ(x) · t(x)ν(x).<br />

M

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