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
Create successful ePaper yourself
Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.
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