Remark 15.112.11. In order to use the inertia character \theta : I \to \mu _ e(\kappa (\mathfrak m)) for infinite Galois extensions, it is convenient to scale it. Let A, K, L, B, \mathfrak m, G, P, I, D, e, \theta be as in Lemma 15.112.5 and Definition 15.112.6. Then e = q |I_ t| with q is a power of the characteristic p of \kappa (\mathfrak m) if positive or 1 if zero. Note that \mu _ e(\kappa (\mathfrak m)) = \mu _{|I_ t|}(\kappa (\mathfrak m)) because the characteristic of \kappa (\mathfrak m) is p. Consider the map
This map induces an isomorphism \theta _{can} : I_ t \to \mu _{|I_ t|}(\kappa (\mathfrak m)). We have \theta _{can}(\tau \sigma \tau ^{-1}) = \tau (\theta _{can}(\sigma )) for \tau \in D and \sigma \in I by Lemma 15.112.7. Finally, if M/L is an extension such that M/K is Galois and \mathfrak m' is a prime of the integral closure of A in M lying over \mathfrak m, then we get the commutative diagram
by Lemma 15.112.10.
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