Inter-universal Teichmuller Theory I: Construction of Hodge Theaters
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