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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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148 SHINICHI MOCHIZUKI<br />

the F l<br />

-symmetry is reminiscent <strong>of</strong> the fact that the multiplicative symmetries <strong>of</strong><br />

the upper half-plane recalled above act transitively on the entire boundary <strong>of</strong> the<br />

upper half-plane. That is to say, taken as a whole, the geometry and coordinate<br />

naturally associated to this multiplicative symmetry <strong>of</strong> the upper half-plane may<br />

be thought <strong>of</strong>, at the level <strong>of</strong> “combinatorial prototypes”, as the geometric<br />

apparatus associated to a node, i.e., <strong>of</strong> the sort that occurs in the reduction modulo<br />

p <strong>of</strong> a Hecke correspondence [cf. the discussion <strong>of</strong> [IUTchII], Remark 4.11.4, (iii),<br />

(c); [NodNon], Introduction]. Finally, we note that, just as in the case <strong>of</strong> the<br />

F ⋊±<br />

l<br />

-, F l<br />

-symmetries discussed in the present paper, the only “coric” symmetries,<br />

i.e., symmetries common to both the additive and multiplicative symmetries <strong>of</strong> the<br />

upper half-plane recalled above, are the symmetries “{±1}” [i.e., the symmetries<br />

z ↦→ z,−z in the case <strong>of</strong> the upper half-plane]. The observations <strong>of</strong> the above<br />

discussion are summarized in Fig. 6.4 below.<br />

Remark 6.12.4.<br />

(i) Just as in the case <strong>of</strong> the F l<br />

-symmetry <strong>of</strong> Proposition 4.9, (i), the F⋊±<br />

l<br />

-<br />

symmetry <strong>of</strong> Proposition 6.8, (i), will eventually be applied, in the theory <strong>of</strong> the<br />

present series <strong>of</strong> papers [cf. theory <strong>of</strong> [IUTchII], [IUTchIII]], to establish an<br />

explicit network <strong>of</strong> comparison isomorphisms<br />

relating various objects — such as log-volumes — associated to the non-labeled<br />

prime-strips that are permuted by this symmetry [cf. the discussion <strong>of</strong> Remark<br />

4.9.1, (i)]. Moreover, just as in the case <strong>of</strong> the F l<br />

-symmetry studied in §4 [cf. the<br />

discussion <strong>of</strong> Remark 4.9.2], one important property <strong>of</strong> this “network <strong>of</strong> comparison<br />

isomorphisms” is that it operates without “label crushing” [cf. Remark 4.9.2, (i)]<br />

— i.e., without disturbing the bijective relationship between the set <strong>of</strong> indices <strong>of</strong><br />

the symmetrized collection <strong>of</strong> prime-strips and the set <strong>of</strong> labels ∈ T → ∼ F l under<br />

consideration. Finally, just as in the situation studied in §4,<br />

this crucial synchronization <strong>of</strong> labels is essentially a consequence <strong>of</strong><br />

the single connected component<br />

— or, at a more abstract level, the single basepoint — <strong>of</strong> the global object [i.e.,<br />

“ † D ⊚± ” in the present §6; “ † D ⊚ ”in§4] that appears in the [D-Θ ±ell -orD-ΘNF-]<br />

<strong>Hodge</strong> theater under consideration [cf. Remark 4.9.2, (ii)].<br />

(ii) At a more concrete level, the “synchronization <strong>of</strong> labels” discussed in (i) is<br />

realized by means <strong>of</strong> the crucial bijections<br />

† ζ : LabCusp( † D ⊚ ) ∼ → J;<br />

† ζ ± : LabCusp ± ( † D ⊚± ) ∼ → T<br />

<strong>of</strong> Propositions 4.7, (iii); 6.5, (iii). Here, we pause to observe that it is precisely the<br />

existence <strong>of</strong> these<br />

bijections relating index sets <strong>of</strong> capsules <strong>of</strong> D-prime-strips to sets <strong>of</strong><br />

global [±-]label classes <strong>of</strong> cusps

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