Paper XI visual guide · Visual 3 of 47 · PART I / FINITE TAME COORDINATES

Fourier projectors isolate tame inertia

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Original source locator: Original Section 3; geometric Frobenius convention

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Let \(t\) generate a finite tame quotient of order \(M\), with \((q,M)=1\). For \(j\in\mathbb Z/M\mathbb Z\) define

\[ P_j=\frac1M\sum_{a=0}^{M-1}\zeta_M^{-ja}r(t)^a, \qquad \zeta_M=e^{2\pi i/M}. \]

The finite Fourier identities give \(P_jP_k=\delta_{jk}P_j\) and \(\sum_jP_j=I\). Thus \(P_jV\) is the \(\zeta_M^j\) character space for \(r(t)\).

The guide uses geometric Frobenius with

\[ \Phi^{-1}r(t)\Phi=r(t)^q. \]

Equivalently \(\Phi r(t)\Phi^{-1}=r(t)^{q^{-1}}\), where the inverse is taken modulo \(M\). Substituting in the Fourier sum gives

\[ \Phi P_j\Phi^{-1}=P_{qj}. \]

Scope

If the forward relation \(\Phi r(t)\Phi^{-1}=r(t)^q\) is used instead, the projector label is \(q^{-1}j\). The two directions have the same orbit sets but different conjugation identities. The release corrects the historical mixed-convention sentence.

Reading the diagram

A packet is an actual eigenspace selected by an idempotent. Frobenius carries it to the next character packet.

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