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10.3 Function o ​ r ​ d l [03WI]

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10.3 Function o​r​dlord_{l}

For l∈ℒl\in{\cal L} we will define an order function

o​r​dl∈Γ⁡((0,+∞),fl∗​(A​f​f𝐙,Y))ord_{l}\in\Gamma((0,+\infty),f_{l}^{\ast}(Aff_{{\bf Z},Y}))

(its meaning will become clear later) by the following inductive procedure:

  1. 1.

    Let l∈ℒi​nl\in{\cal L}_{in} and t>0t>0 be sufficiently small. Then in the standard affine coordinates near s=fl​(0)s=f_{l}(0) one has αl=±fl∗​(d​y)\alpha_{l}=\pm f_{l}^{\ast}(dy). We define o​r​dl=±fl∗​(y)ord_{l}=\pm f_{l}^{\ast}(y). Then d⁡(o​r​dl)=αld(ord_{l})=\alpha_{l}, and we can extend uniquely o​r​dlord_{l} for all t∈(0,+∞)t\in(0,+\infty).

  2. 2.

    Let l∈ℒc​o​ml\in{\cal L}_{com} and l1,l2l_{1},l_{2} be parents of ll. In the notation of Axiom 3 we have fl1​(t1)=fl2​(t2)=fl​(0)f_{l_{1}}(t_{1})=f_{l_{2}}(t_{2})=f_{l}(0) and αl​(0)=n1​αl1​(t1)+n2​αl2​(t2)\alpha_{l}(0)=n_{1}\alpha_{l_{1}}(t_{1})+n_{2}\alpha_{l_{2}}(t_{2}). Then we define o​r​dl​(0):=n1​o​r​dl1​(t1)+n2​o​r​dl2​(t2)ord_{l}(0):=n_{1}ord_{l_{1}}(t_{1})+n_{2}ord_{l_{2}}(t_{2}). Again, using the condition d⁡(o​r​dl)=αld(ord_{l})=\alpha_{l} and the knowledge of o​r​dl​(0)ord_{l}(0) we can extend o​r​dlord_{l} for t>0t>0.

Notice that o​r​dl​(t)ord_{l}(t) can be thought of as affine function on the tangent space Tfl​(t)​YT_{f_{l}(t)}Y (in the induced integral affine structure). In particular, we have a half-plane Pl,t⊂Tfl​(t)​YP_{l,t}\subset T_{f_{l}(t)}Y defined by the inequality o​r​dl​(t)>0ord_{l}(t)>0. The family of half-planes Pl,tP_{l,t} is covariantly constant with respect to ∇a​f​f\nabla^{aff}.

Each half-plane Pl,tP_{l,t} contains 0∈Tfl​(t)​Y0\in T_{f_{l}(t)}Y strictly in its interior. Recall that at the end of Section 9.1 we defined another half-plane Pl,t(0)⊂Tfl​(t)​YP_{l,t}^{(0)}\subset T_{f_{l}(t)}Y. It is easy to see that Pl,t(0)P_{l,t}^{(0)} is the half-plane parallel to Pl,tP_{l,t} such that 0∈Tfl​(t)​Y0\in T_{f_{l}(t)}Y is on the boundary of Pl,t(0)P_{l,t}^{(0)}.

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