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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18 SHINICHI MOCHIZUKI<br />
If one thinks <strong>of</strong> the geometry <strong>of</strong> “conventional scheme theory” as being analogous<br />
to the geometry <strong>of</strong> “Euclidean space”, then the geometry represented by the<br />
Frobenius-picture corresponds to a “topological manifold”, i.e., which is obtained by<br />
gluing together various portions <strong>of</strong> Euclidean space, but which is not homeomorphic<br />
to Euclidean space. This point <strong>of</strong> view is illustrated in Fig. I2.1 above, where the<br />
various Θ ±ell NF-<strong>Hodge</strong> theaters in the Frobenius-picture are depicted as [twodimensional!<br />
— cf. the discussion <strong>of</strong> §I1] twice-punctured topological surfaces<br />
<strong>of</strong> genus one, glued together along tubular neighborhoods <strong>of</strong> cycles, which<br />
correspond to the [one-dimensional! — cf. the discussion <strong>of</strong> §I1] mono-analytic<br />
data that appears in the isomorphism that constitutes the Θ-link. The permutation<br />
symmetries in the étale-picture [cf. the discussion <strong>of</strong> §I1] are depicted in Fig.<br />
I2.1 as the anti-holomorphic reflection [cf. the discussion <strong>of</strong> multiradiality in<br />
[IUTchII], Introduction!] around a gluing cycle between topological surfaces.<br />
Another elementary example that illustrates the spirit <strong>of</strong> the gluing operations<br />
discussed in the present series <strong>of</strong> papers is the following. For i =0, 1, let R i be<br />
acopy<strong>of</strong>thereal line; I i ⊆ R i the closed unit interval [i.e., corresponding to<br />
[0, 1] ⊆ R]. Write C 0 ⊆ I 0 for the Cantor set and<br />
φ : C 0<br />
∼<br />
→ I1<br />
for the bijection arising from the Cantor function. Thenifonethinks<strong>of</strong>R 0 and<br />
R 1 as being glued to one another by means <strong>of</strong> φ, thenitisahighly nontrivial<br />
problem<br />
to describe structures naturally associated to the “alien” ring structure<br />
<strong>of</strong> R 0 — such as, for instance, the subset <strong>of</strong> algebraic numbers ∈ R 0 —<br />
in terms that only require the use <strong>of</strong> the ring structure <strong>of</strong> R 1 .<br />
A slightly less elementary example that illustrates the spirit <strong>of</strong> the gluing operations<br />
discussed in the present series <strong>of</strong> papers is the following. This example is<br />
technically much closer to the theory <strong>of</strong> the present series <strong>of</strong> papers than the examples<br />
involving topological surfaces and Cantor sets given above. For simplicity, let<br />
us write<br />
G O × , G O ⊲<br />
for the pairs “G v O × ”, “G<br />
F v<br />
v<br />
O ⊲ ” [cf. the notation <strong>of</strong> the discussion<br />
F v<br />
surrounding Fig. I1.2]. Recall from [AbsTopIII], Proposition 3.2, (iv), that the<br />
operation<br />
(G O ⊲ ) ↦→ G<br />
<strong>of</strong> “forgetting O ⊲ ” determines a bijection from the group <strong>of</strong> automorphisms <strong>of</strong><br />
the pair G O ⊲ — i.e., thought <strong>of</strong> as an abstract topological monoid equipped<br />
with a continuous action by an abstract topological group — to the group <strong>of</strong> automorphisms<br />
<strong>of</strong> the topological group G. By contrast, we recall from [AbsTopIII],<br />
Proposition 3.3, (ii), that the operation<br />
(G O × ) ↦→ G<br />
<strong>of</strong> “forgetting O × ” only determines a surjection from the group <strong>of</strong> automorphisms<br />
<strong>of</strong> the pair G O × — i.e., thought <strong>of</strong> as an abstract topological monoid equipped