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Explicit Estimates in Inter-universal Teichm¨ uller Theory (joint work w/ S. Mochizuki, I. Fesenko, Y. Hoshi, and

W. Porowski)

Arata Minamide

RIMS, Kyoto University

September 7, 2021

Notations Log-volume IUTchIV Vojta ABC (ii) Lem Goal Theta Heights Auxiliary Main

Arata Minamide (RIMS, Kyoto University) Explicits Estimates in IUTch September 7, 2021 1 / 34

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Notations

Primes: the set of all prime numbers

F: a number field ⊇ OF: the ring of integers

F: the absolute value of the discriminant ofF V(F)non: the set of nonarchimedean places ofF V(F)arc: the set of archimedean places ofF V(F) def= V(F)non

V(F)arc

For v∈V(F), writeFv for the completion ofF atv

For v∈V(F)non, writepv⊆ OF for the prime ideal corr. tov

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Let v∈V(F)non. Writeordv :F×↠Z for the order def’d byv.

Then for any x∈F, we shall write

|x|v

def= ♯(OF/pv)ordv(x).

Let v∈V(F)arc. Writeσv :F ,→Cfor the embed. det’d, up to complex conjugation, byv. Then for any x∈F, we shall write

|x|v

def= v(x)|[FCv:R].

Note: (Product formula) Forα∈F×, it holds that

v∈V(F)

|α|v = 1.

For an elliptic curveE /a field, writej(E) for the j-invariant of E

Arata Minamide (RIMS, Kyoto University) Explicits Estimates in IUTch September 7, 2021 3 / 34

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Log-volume estimates for Θ-pilot objects (cf. [IUTchIII], Cor 3.12)

Theorem Write

−|log(Θ)| ∈ R∪ {∞}

for the (process.-normalized, mono-an.) log-volume of the “holomorphic hull” of theunion of the possible images of a Θ-pilot object, rel. to the relevant Kum. isoms, in the multira’l rep’n of [IUTchIII], Thm 3.11, (i), which we regard as sub. to (Ind1), (Ind2), (Ind3);

−|log(q)| ∈ R

for the (process.-normalized, mono-an.) log-volume of the image of a q-pilot object, rel. to the relevant Kum. isoms, in the multirad’l rep’n. Then it holds that −|log(Θ)| ∈R, and −|log(Θ)| ≥ −|log(q)|.

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Log-volume estimates for Θ-pilot objects (cf. [IUTchIII], Cor 3.12)

Theorem Write

−|log(Θ)| ∈ R∪ {∞}

for the (process.-normalized, mono-an.) log-volume of the “holomorphic hull” of theunion of the possible images of a Θ-pilot object, rel. to the relevant Kum. isoms, in the multira’l rep’n of [IUTchIII], Thm 3.11, (i), which we regard as sub. to (Ind1), (Ind2), (Ind3);

−|log(q)| ∈ R

for the (process.-normalized, mono-an.) log-volume of the image of a q-pilot object, rel. to the relevant Kum. isoms, in the multirad’l rep’n.

Then it holds that −|log(Θ)| ∈R, and −|log(Θ)| ≥ −|log(q)|.

Arata Minamide (RIMS, Kyoto University) Explicits Estimates in IUTch September 7, 2021 4 / 34

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Log-volume estimates for Θ-pilot objects (cf. [IUTchIII], Cor 3.12)

Theorem Write

−|log(Θ)| ∈ R∪ {∞}

for the (process.-normalized, mono-an.) log-volume of the “holomorphic hull” of theunion of the possible images of a Θ-pilot object, rel. to the relevant Kum. isoms, in the multira’l rep’n of [IUTchIII], Thm 3.11, (i), which we regard as sub. to (Ind1), (Ind2), (Ind3);

−|log(q)| ∈ R

for the (process.-normalized, mono-an.) log-volume of the image of a q-pilot object, rel. to the relevant Kum. isoms, in the multirad’l rep’n.

Then it holds that −|log(Θ)| ∈R, and −|log(Θ)| ≥ −|log(q)|.

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Results in [IUTchIV]

For λ Q\ {0,1},

Aλ: the elliptic curve/Q(λ) def’d by “y2 =x(x−1)(x−λ)”

Fλ def= Q(λ,

1, Aλ[3·5](Q))

Eλ def= Aλ×Q(λ)Fλ has at mostsplit multipl. red. at ∀ ∈V(Fλ) qλ: the arithmetic divisor det’d by theq-parameters of Eλ/Fλ fλ: the “reduced” arithmetic divisor det’d byqλ

dλ: the arithmetic divisor det’d by the different ofFλ/Q

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Theorem (Vojta Conj. — in the case of P1\ {0,1,∞}— for “K”) Let d∈Z>0,ϵ∈R>0R1,

K ⊆ Q\ {0,1}: acompactly bounded subset whose “support”2,. Then B(d, ϵ,K)R>0 — that depends only ond,ϵ, and K — s.t.

the function on Kddef= {λ∈ K | [Q(λ) :Q]≤d}given by λ 7→ 16·deg(qλ)(1 +ϵ)·(deg(dλ) + deg(fλ)) is bounded by B(d, ϵ,K).

Proof: By applying

the finiteness of {λ∈ Kd | deg(qλ)≤γ}R>0) (cf. Northcott’s theorem),

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Theorem (Vojta Conj. — in the case of P1\ {0,1,∞}— for “K”) Let d∈Z>0,ϵ∈R>0R1,

K ⊆ Q\ {0,1}: acompactly bounded subset whose “support”2,. Then B(d, ϵ,K)R>0 — that depends only ond,ϵ, and K — s.t.

the function on Kddef= {λ∈ K | [Q(λ) :Q]≤d}given by λ 7→ 16·deg(qλ)(1 +ϵ)·(deg(dλ) + deg(fλ)) is bounded by B(d, ϵ,K).

Proof: By applying

the finiteness of {λ∈ Kd | deg(qλ)≤γ}R>0) (cf. Northcott’s theorem),

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♯{j(“arithmetic” elliptic curve over a field of char. zero)}= 4 (cf. Takeuchi’s list),

the prime number theorem,

the theory of Galois actions on torsion points of elliptic curves (cf. [GenEll]),

we conclude that for all butfinitely many λ∈ Kd, there exists a prime number lλ such that

(i) an initialΘ-data(Q/Fλ, Eλ, lλ, . . .) s.t. Eλ hasgood red. at every V(Fλ)goodV(Fλ)non that does not divide 2lλ

(In the following, we shall write

qbadλ : the arithmetic divisor det’d by “restricting qλ toVbadmod”.)

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♯{j(“arithmetic” elliptic curve over a field of char. zero)}= 4 (cf. Takeuchi’s list),

the prime number theorem,

the theory of Galois actions on torsion points of elliptic curves (cf. [GenEll]),

we conclude that for all butfinitely many λ∈ Kd, there exists a prime number lλ such that

(i) an initialΘ-data(Q/Fλ, Eλ, lλ, . . .) s.t. Eλ hasgood red.

at every V(Fλ)goodV(Fλ)non that does not divide 2lλ (In the following, we shall write

qbadλ : the arithmetic divisor det’d by “restricting qλ toVbadmod”.)

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(ii) 16 ·deg(qbadλ ) (1 + 20dl λ

λ )·(deg(dλ) + deg(fλ)) + 20·δλ·lλ, wheredλ := [Q(λ) :Q],δλ := 212·33·5·dλ (cf. (i); “Cor 3.12”) (iii) ordlλ(q) < deg(qλ)1/2, whereV(Fλ)□|lλ

(iv) deg(qλ)1/2 lλ 10·δ·deg(qλ)1/2·log(2·δ·deg(qλ)) whereδ := 212·33·5·d

Then it follows from (i), (iii) [cf. also the “compactness” of K] that λ 7→ 16deg(qλ)16deg(qbadλ )deg(qλ)1/2log(2δdeg(qλ)) is bounded. On the other hand, it follows from (ii), (iv) that

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(ii) 16 ·deg(qbadλ ) (1 + 20dl λ

λ )·(deg(dλ) + deg(fλ)) + 20·δλ·lλ, wheredλ := [Q(λ) :Q],δλ := 212·33·5·dλ (cf. (i); “Cor 3.12”) (iii) ordlλ(q) < deg(qλ)1/2, whereV(Fλ)□|lλ

(iv) deg(qλ)1/2 lλ 10·δ·deg(qλ)1/2·log(2·δ·deg(qλ)) whereδ := 212·33·5·d

Then it follows from (i), (iii) [cf. also the “compactness” of K] that λ 7→ 16deg(qλ)16deg(qbadλ )deg(qλ)1/2log(2δdeg(qλ)) is bounded. On the other hand, it follows from (ii), (iv) that

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1

6deg(qbadλ ) (1 +δ·deg(qλ)1/2)(deg(dλ) + deg(fλ)) + 200δ2·deg(qλ)1/2log(2δdeg(qλ)).

In particular, these two displays imply that λ7→ (125(60δ)2deg(qlog(2δdeg(qλ))

λ)1/2 )16deg(qλ)(1 +deg(qδ

λ)1/2)(deg(dλ) + deg(fλ)) is bounded. By enlarging our “exceptional set”, we conclude that

λ 7→ 16 ·deg(qλ)(1 +ϵ)·(deg(dλ) + deg(fλ)) is bounded. This completes the proof of Theorem.

Then, by applying the theory of noncritical Belyi maps, we obtain (): the “version withK removed” of Theorem (cf. [GenEll]).

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1

6deg(qbadλ ) (1 +δ·deg(qλ)1/2)(deg(dλ) + deg(fλ)) + 200δ2·deg(qλ)1/2log(2δdeg(qλ)).

In particular, these two displays imply that λ7→

(125(60δ)2deg(qlog(2δdeg(qλ))

λ)1/2 )16deg(qλ)(1 + δ

deg(qλ)1/2)(deg(dλ) + deg(fλ)) is bounded.

By enlarging our “exceptional set”, we conclude that λ 7→ 16 ·deg(qλ)(1 +ϵ)·(deg(dλ) + deg(fλ)) is bounded. This completes the proof of Theorem.

Then, by applying the theory of noncritical Belyi maps, we obtain (): the “version withK removed” of Theorem (cf. [GenEll]).

Arata Minamide (RIMS, Kyoto University) Explicits Estimates in IUTch September 7, 2021 9 / 34

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1

6deg(qbadλ ) (1 +δ·deg(qλ)1/2)(deg(dλ) + deg(fλ)) + 200δ2·deg(qλ)1/2log(2δdeg(qλ)).

In particular, these two displays imply that λ7→

(125(60δ)2deg(qlog(2δdeg(qλ))

λ)1/2 )16deg(qλ)(1 + δ

deg(qλ)1/2)(deg(dλ) + deg(fλ)) is bounded. By enlarging our “exceptional set”, we conclude that

λ 7→ 16·deg(qλ)(1 +ϵ)·(deg(dλ) + deg(fλ)) is bounded. This completes the proof of Theorem.

Then, by applying the theory of noncritical Belyi maps, we obtain (): the “version withK removed” of Theorem (cf. [GenEll]).

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1

6deg(qbadλ ) (1 +δ·deg(qλ)1/2)(deg(dλ) + deg(fλ)) + 200δ2·deg(qλ)1/2log(2δdeg(qλ)).

In particular, these two displays imply that λ7→

(125(60δ)2deg(qlog(2δdeg(qλ))

λ)1/2 )16deg(qλ)(1 + δ

deg(qλ)1/2)(deg(dλ) + deg(fλ)) is bounded. By enlarging our “exceptional set”, we conclude that

λ 7→ 16·deg(qλ)(1 +ϵ)·(deg(dλ) + deg(fλ)) is bounded. This completes the proof of Theorem.

Then, by applying the theory of noncritical Belyi maps, we obtain (): the “version withK removed” of Theorem (cf. [GenEll]).

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Theorem (Corollary of () — ABC Conjecture for number fields) Let d∈Z>0,ϵ∈R>0R1.

Then C(d, ϵ)∈R>0 — that depends only on dandϵ— s.t. for

F: a number field — whered = [F :Q]

(a, b, c) : a triple of elements∈F× — wherea+b+c= 0 we have

HF(a, b, c) < C(d, ϵ)·(∆F ·radF(a, b, c))1+ϵ

— where

HF(a, b, c) def= ∏

v∈V(F)max{|a|v,|b|v,|c|v}, radF(a, b, c) def= ∏

{v∈V(F)non|{|a|v,|b|v,|c|v}≥2}♯(OF/pv).

Note: We do not know the constant “C(d, ϵ)” explicitly.

For instance, it is hard to compute noncritical Belyi mapsexplicitly.

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Theorem (Corollary of () — ABC Conjecture for number fields) Let d∈Z>0,ϵ∈R>0R1.

Then C(d, ϵ)∈R>0 — that depends only on dandϵ— s.t. for

F: a number field — whered = [F :Q]

(a, b, c) : a triple of elements∈F× — wherea+b+c= 0 we have

HF(a, b, c) < C(d, ϵ)·(∆F ·radF(a, b, c))1+ϵ

— where

HF(a, b, c) def= ∏

v∈V(F)max{|a|v,|b|v,|c|v}, radF(a, b, c) def= ∏

{v∈V(F)non|{|a|v,|b|v,|c|v}≥2}♯(OF/pv).

Note: We do not know the constant “C(d, ϵ)”explicitly.

For instance, it is hard to compute noncritical Belyi mapsexplicitly.

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Computations concerning (ii)

For γ R, we shall write ⌊γ⌋ (resp. ⌈γ⌉) for the largest integer

γ (resp. the smallest integer γ).

{ki}iI: a finite set of p-adic local fields (Oki: the ring of integers) ei (resp. di): the abs. ram. index (resp. the order of an gen. of δki)

aidef= {1

eipei2 (p >2)

2 (p= 2) bidef= log(plog(p)·ei/(p1))⌋ −e1i aIdef

= ∑

iI

ai, bI def

= ∑

iI

bi, dI def

= ∑

iI

di

µlogk

I: the (nor’d) log-vol. on kI def= iIki s.t. µlogk

I (iIOki) = 0

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Lemma

For λ∈ e1iZ, write pλOki for the fractional ideal generated by any element x∈ki s.t. ord(x) =λ. Let

ϕ:QpZp

iI

logp(Ok×i) QpZp

iI

logp(Ok×i)

be an automorphismof the finite dimensional Qp-vector space that induces an automorphism of the submodule

iIlogp(Ok×i).

(i) WriteIdef= {i∈I |ei > p−2}. For any λ∈ e1i

0Z, i0 ∈I, ϕ(pλ(iIOki)) ∪

pλ

iI 1

2plogp(Ok×i)

pλdIaI

iI

logp(O×ki) pλdIaI⌋−bI(iIOki).

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Lemma

For λ∈ e1iZ, write pλOki for the fractional ideal generated by any element x∈ki s.t. ord(x) =λ. Let

ϕ:QpZp

iI

logp(Ok×i) QpZp

iI

logp(Ok×i)

be an automorphismof the finite dimensional Qp-vector space that induces an automorphism of the submodule

iIlogp(Ok×i).

(i) WriteIdef= {i∈I |ei > p−2}. For any λ∈ e1i

0Z, i0 ∈I, ϕ(pλ(⊗iIOki)) ∪

pλ

iI 1

2plogp(Ok×i)

pλdIaI

iI

logp(O×ki) pλdIaI⌋−bI(iIOki).

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Moreover, we have µlogk

I(pλdIaI⌋−bI(i∈IOki))

(−λ+dI+ 1) log(p) +∑

iI

(3 + log(ei)).

(ii) Suppose that p >2 and ei= 1 (i∈I). Then ϕ((⊗iIOki))

iI 1

2plogp(Ok×i) = (iIOki). Moreover, we have

µlogk

I((⊗iIOki)) = 0.

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Moreover, we have µlogk

I(pλdIaI⌋−bI(i∈IOki))

(−λ+dI+ 1) log(p) +∑

iI

(3 + log(ei)).

(ii) Suppose that p >2 and ei= 1 (i∈I). Then ϕ((⊗iIOki))

iI 1

2plogp(Ok×i) = (iIOki). Moreover, we have

µlogk

I((⊗iIOki)) = 0.

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In the following discussion, for simplicity, write

(F /F, E, l, . . .) def= (Q/Fλ, Eλ, lλ, . . .).

( K =F(E[l]) F Fmod: the field of moduli ofE)

dmod def= [Fmod:Q] emod def= the max. ram. index of Fmod/Q dmod def= 212·33·5·dmod emod def= 212·33·5·emod

VnonQ def= V(Q)non VdstQ def= {vQ VnonQ |vQ ramifies inK} Let us compute an upper boundfor the

(process.-normalized, mono-an.) log-volume of the “holomorphic hull” of the union of the possible images of aΘ-pilot object, rel. to the relevant Kum. isoms, in the multira’l rep’n of [IUTchIII], Thm 3.11, (i), which we regard as sub. to (Ind1), (Ind2), (Ind3)

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In the following discussion, for simplicity, write

(F /F, E, l, . . .) def= (Q/Fλ, Eλ, lλ, . . .).

( K =F(E[l]) F Fmod: the field of moduli ofE)

dmod def= [Fmod:Q] emod def= the max. ram. index of Fmod/Q dmod def= 212·33·5·dmod emod def= 212·33·5·emod

VnonQ def= V(Q)non VdstQ def= {vQ VnonQ |vQ ramifies in K}

Let us compute an upper boundfor the

(process.-normalized, mono-an.) log-volume of the “holomorphic hull” of the union of the possible images of aΘ-pilot object, rel. to the relevant Kum. isoms, in the multira’l rep’n of [IUTchIII], Thm 3.11, (i), which we regard as sub. to (Ind1), (Ind2), (Ind3)

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In the following discussion, for simplicity, write

(F /F, E, l, . . .) def= (Q/Fλ, Eλ, lλ, . . .).

( K =F(E[l]) F Fmod: the field of moduli ofE)

dmod def= [Fmod:Q] emod def= the max. ram. index of Fmod/Q dmod def= 212·33·5·dmod emod def= 212·33·5·emod

VnonQ def= V(Q)non VdstQ def= {vQ VnonQ |vQ ramifies in K} Let us compute an upper boundfor the

(process.-normalized, mono-an.) log-volume of the “holomorphic hull” of the union of the possible images of aΘ-pilot object, rel.

to the relevant Kum. isoms, in the multira’l rep’n of [IUTchIII], Thm 3.11, (i), which we regard as sub. to (Ind1), (Ind2), (Ind3)

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(A) Let vQVdstQ . Fix j (∈ {1,2, . . . , l}) and the collection {vi}i∈S±

j+1

of [not necessarily distinct] elements of V(Fmod)vQ. Write vi V

V(Fmod) for the elem’t corr. to vi.

Then, by applying Lem, (i), we obtain an upper boundon the component of the log-volume in question corresponding to the tensor product of the Q-spans of the log-shells associated to the collection {vi}i∈S±

j+1 as follows: (−λ+dI+ 1) log(pvQ) + 4(j+ 1)ιvQlog(emod·l)

— whereλ = {j2

2lord(qvj) (vj Vbad)

0 (vj Vgood) ιvQ = {

1 (pvQ ≤emodl) 0 (pvQ > emodl)

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(A) Let vQVdstQ . Fix j (∈ {1,2, . . . , l}) and the collection {vi}i∈S±

j+1

of [not necessarily distinct] elements of V(Fmod)vQ. Write vi V

V(Fmod) for the elem’t corr. to vi. Then, by applying Lem, (i), we obtain an upper boundon the component of the log-volume in question corresponding to the tensor product of the Q-spans of the log-shells associated to the collection {vi}i∈S±

j+1 as follows:

(−λ+dI+ 1) log(pvQ) + 4(j+ 1)ιvQlog(emod·l)

— whereλ = {j2

2lord(qvj) (vj Vbad)

0 (vj Vgood) ιvQ = {

1 (pvQ ≤emodl) 0 (pvQ > emodl)

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(A) Let vQVdstQ . Fix j (∈ {1,2, . . . , l}) and the collection {vi}i∈S±

j+1

of [not necessarily distinct] elements of V(Fmod)vQ. Write vi V

V(Fmod) for the elem’t corr. to vi. Then, by applying Lem, (i), we obtain an upper boundon the component of the log-volume in question corresponding to the tensor product of the Q-spans of the log-shells associated to the collection {vi}i∈S±

j+1 as follows:

(−λ+dI+ 1) log(pvQ) + 4(j+ 1)ιvQlog(emod·l)

— whereλ = {j2

2lord(qvj) (vj Vbad)

0 (vj Vgood) ιvQ = {

1 (pvQ ≤emodl) 0 (pvQ > emodl)

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(B) Let vQVnonQ \VdstQ . Fix j (∈ {1,2, . . . , l}) and {vi}i∈S± j+1

as in (A).

Then, by applying Lem, (ii), we obtain an upper boundon the comp. of the log-vol. in question corr. to the tensor prod. of the Q-spans of the log-shells assoc. to {vi}i∈S±

j+1 as follows: 0

(C) Let vQ VarcQ . Fix j (∈ {1,2, . . . , l}) and {vi}i∈S±

j+1 as in (A). Then we obtain an upper boundon the comp. of the log-vol. in question corr. to the tensor prod. of the Q-spans of the log-shells assoc. to {vi}i∈S±

j+1 as follows:

(j+ 1)·log(π)

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(B) Let vQVnonQ \VdstQ . Fix j (∈ {1,2, . . . , l}) and {vi}i∈S± j+1

as in (A). Then, by applying Lem, (ii), we obtain an upper boundon the comp. of the log-vol. in question corr. to the tensor prod. of the Q-spans of the log-shells assoc. to {vi}i∈S±

j+1 as follows:

0

(C) Let vQ VarcQ . Fix j (∈ {1,2, . . . , l}) and {vi}i∈S±

j+1 as in (A). Then we obtain an upper boundon the comp. of the log-vol. in question corr. to the tensor prod. of the Q-spans of the log-shells assoc. to {vi}i∈S±

j+1 as follows:

(j+ 1)·log(π)

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(B) Let vQVnonQ \VdstQ . Fix j (∈ {1,2, . . . , l}) and {vi}i∈S± j+1

as in (A). Then, by applying Lem, (ii), we obtain an upper boundon the comp. of the log-vol. in question corr. to the tensor prod. of the Q-spans of the log-shells assoc. to {vi}i∈S±

j+1 as follows:

0

(C) Let vQ VarcQ . Fix j (∈ {1,2, . . . , l}) and {vi}i∈S±

j+1 as in (A). Then we obtain an upper boundon the comp. of the log-vol. in question corr. to the tensor prod. of the Q-spans of the log-shells assoc. to {vi}i∈S±

j+1 as follows:

(j+ 1)·log(π)

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(B) Let vQVnonQ \VdstQ . Fix j (∈ {1,2, . . . , l}) and {vi}i∈S± j+1

as in (A). Then, by applying Lem, (ii), we obtain an upper boundon the comp. of the log-vol. in question corr. to the tensor prod. of the Q-spans of the log-shells assoc. to {vi}i∈S±

j+1 as follows:

0

(C) Let vQ VarcQ . Fix j (∈ {1,2, . . . , l}) and {vi}i∈S±

j+1 as in (A). Then we obtain an upper boundon the comp. of the log-vol.

in question corr. to the tensor prod. of the Q-spans of the log-shells assoc. to {vi}i∈S±

j+1 as follows:

(j+ 1)·log(π)

(35)

After computing a “weighted average upper bound”, i.e., ([F 1

mod:Q])j+1

v0,... ,vj∈V(Fmod)vQ

0ij

[(Fmod)vi :QvQ]()

and then a “procession-normalized upper bound”, i.e.,

1 l

1jl

()

for eachvQ VQ, by summing over vQ VQ these estimates, we obtain anupper boundon −|log(Θ)| as follows:

l+1 4

{

(1 + 12dlmod)·(deg(dλ) + deg(fλ)) + 10·emod·l

16 ·(112l2)·log(qbadλ )

} 2l1 ·deg(qbadλ )

Arata Minamide (RIMS, Kyoto University) Explicits Estimates in IUTch September 7, 2021 17 / 34

(36)

After computing a “weighted average upper bound”, i.e., ([F 1

mod:Q])j+1

v0,... ,vj∈V(Fmod)vQ

0ij

[(Fmod)vi :QvQ]()

and then a “procession-normalized upper bound”, i.e.,

1 l

1jl

()

for eachvQ VQ, by summing over vQ VQ these estimates, we obtain anupper boundon −|log(Θ)| as follows:

l+1 4

{

(1 +12dlmod)·(deg(dλ) + deg(fλ)) + 10·emod·l

16 ·(112l2)·log(qbadλ )

}2l1 ·deg(qbadλ )

(37)

On the other hand, since −|log(Θ)| ≥ −|log(q)|=2l1 ·deg(qbadλ ), we conclude that

1

6 ·(1 12l2)·deg(qbadλ )

(1 +12dlmod)·(deg(dλ) + deg(fλ)) + 10·emod·l, hence that

1

6 ·deg(qbadλ ) (1 +20dmodl )·(deg(dλ) + deg(fλ)) + 20·dmod·l.

Arata Minamide (RIMS, Kyoto University) Explicits Estimates in IUTch September 7, 2021 18 / 34

(38)

On the other hand, since −|log(Θ)| ≥ −|log(q)|=2l1 ·deg(qbadλ ), we conclude that

1

6 ·(1 12l2)·deg(qbadλ )

(1 +12dlmod)·(deg(dλ) + deg(fλ)) + 10·emod·l,

hence that

1

6 ·deg(qbadλ ) (1 +20dmodl )·(deg(dλ) + deg(fλ)) + 20·dmod·l.

(39)

On the other hand, since −|log(Θ)| ≥ −|log(q)|=2l1 ·deg(qbadλ ), we conclude that

1

6 ·(1 12l2)·deg(qbadλ )

(1 +12dlmod)·(deg(dλ) + deg(fλ)) + 10·emod·l, hence that

1

6 ·deg(qbadλ ) (1 +20dlmod)·(deg(dλ) + deg(fλ)) + 20·dmod·l.

Arata Minamide (RIMS, Kyoto University) Explicits Estimates in IUTch September 7, 2021 18 / 34

(40)

Goal of this joint work:

Under certain conditions, we prove () directly [i.e., without applying the theory of noncritical Belyi maps] to compute the constant “C(d, ϵ)” explicitly.

Technical Difficulties of Explicit Computations

(i) We cannot use the compactness of “K” at the place2

We develop the theory of´etale theta functions so that it functions properly at the place 2

(ii) We cannot use the compactness of “K” at the place

By restricting our attention to special number fields, we

“bound” thearchimedeanportion of the “height” of the elliptic curveEλ

(41)

Goal of this joint work: Under certain conditions, we prove () directly [i.e., without applying the theory of noncritical Belyi maps] to compute the constant “C(d, ϵ)” explicitly.

Technical Difficulties of Explicit Computations

(i) We cannot use the compactness of “K” at the place2

We develop the theory of´etale theta functions so that it functions properly at the place 2

(ii) We cannot use the compactness of “K” at the place

By restricting our attention to special number fields, we

“bound” thearchimedeanportion of the “height” of the elliptic curveEλ

Arata Minamide (RIMS, Kyoto University) Explicits Estimates in IUTch September 7, 2021 19 / 34

(42)

Goal of this joint work: Under certain conditions, we prove () directly [i.e., without applying the theory of noncritical Belyi maps] to compute the constant “C(d, ϵ)” explicitly.

Technical Difficulties of Explicit Computations

(i) We cannot use the compactness of “K” at the place2

We develop the theory of´etale theta functions so that it functions properly at the place 2

(ii) We cannot use the compactness of “K” at the place

By restricting our attention to special number fields, we

“bound” thearchimedeanportion of the “height” of the elliptic curveEλ

(43)

Goal of this joint work: Under certain conditions, we prove () directly [i.e., without applying the theory of noncritical Belyi maps] to compute the constant “C(d, ϵ)” explicitly.

Technical Difficulties of Explicit Computations

(i) We cannot use the compactness of “K” at the place2

We develop the theory of´etale theta functions so that it functions properly at the place2

(ii) We cannot use the compactness of “K” at the place

By restricting our attention to special number fields, we

“bound” thearchimedeanportion of the “height” of the elliptic curveEλ

Arata Minamide (RIMS, Kyoto University) Explicits Estimates in IUTch September 7, 2021 19 / 34

(44)

Goal of this joint work: Under certain conditions, we prove () directly [i.e., without applying the theory of noncritical Belyi maps] to compute the constant “C(d, ϵ)” explicitly.

Technical Difficulties of Explicit Computations

(i) We cannot use the compactness of “K” at the place2

We develop the theory of´etale theta functions so that it functions properly at the place2

(ii) We cannot use the compactness of “K” at the place

By restricting our attention to special number fields, we

“bound” thearchimedeanportion of the “height” of the elliptic curveEλ

(45)

Etale Theta Functions´

p,l: distinct prime numbers — wherel≥5 k: a p-adic local field ⊇ Ok: the ring of integers X: an elliptic curve/k which has split multipl. red. /Ok

q ∈ Ok: the q-parameter of X

Xlog def= (X,{o} ⊆X): the smooth log curve/k assoc. toX In the following, we assume that

√−1 k

X[2l](k) = X[2l](k) [Xlog/{±1}]is a k-core

Arata Minamide (RIMS, Kyoto University) Explicits Estimates in IUTch September 7, 2021 20 / 34

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