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Inter-universal Teichmuller Theory I: Construction of Hodge Theaters

Inter-universal Teichmuller Theory I: Construction of Hodge Theaters

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10 SHINICHI MOCHIZUKI<br />

Classical<br />

upper half-plane<br />

Θ ±ell NF-<strong>Hodge</strong> theaters<br />

in inter-<strong>universal</strong><br />

Teichmüller theory<br />

Additive z ↦→ z + a, F ⋊±<br />

l<br />

-<br />

symmetry z ↦→ −z + a (a ∈ R) symmetry<br />

“Functions” assoc’d<br />

to add. symm.<br />

q def<br />

= e 2πiz theta fn. evaluated at<br />

l-tors. [cf. I, 6.12.6, (ii)]<br />

Basepoint assoc’d single cusp V ±<br />

to add. symm. at infinity [cf. I, 6.1, (v)]<br />

Combinatorial<br />

prototype assoc’d cusp cusp<br />

to add. symm.<br />

Multiplicative<br />

symmetry<br />

z ↦→ z·cos(t)−sin(t)<br />

z·sin(t)+cos(t) , F l -<br />

z ↦→ z·cos(t)+sin(t)<br />

z·sin(t)−cos(t)<br />

(t ∈ R) symmetry<br />

“Functions”<br />

assoc’d to<br />

mult. symm.<br />

w def<br />

= z−i<br />

z+i<br />

elements <strong>of</strong> the<br />

number field F mod<br />

[cf. I, 6.12.6, (iii)]<br />

Basepoints assoc’d<br />

( cos(t) −sin(t)<br />

) (<br />

sin(t) cos(t) , cos(t) sin(t)<br />

)<br />

sin(t) −cos(t)<br />

F l<br />

V Bor = F l<br />

· V ±un<br />

to mult. symm. {entire boundary <strong>of</strong> H } [cf. I, 4.3, (i)]<br />

Combinatorial nodes <strong>of</strong> mod p nodes <strong>of</strong> mod p<br />

prototype assoc’d Hecke correspondence Hecke correspondence<br />

to mult. symm. [cf. II, 4.11.4, (iii), (c)] [cf. II, 4.11.4, (iii), (c)]<br />

Fig. I1.4: Comparison <strong>of</strong> F ⋊±<br />

l<br />

-, F l -symmetries<br />

with the geometry <strong>of</strong> the upper half-plane<br />

As discussed above in our explanation <strong>of</strong> the models at v ∈ V bad for F ⊢ -primestrips,<br />

by considering the 2l-th roots <strong>of</strong> the q-parameters <strong>of</strong> the elliptic curve E F

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