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Some effective estimates for André–Oort in Y(1) n

  • Gal Binyamini ORCID logo and Emmanuel Kowalski
Published/Copyright: September 11, 2019

Abstract

Let X Y ( 1 ) n be a subvariety defined over a number field 𝔽 and let ( P 1 , , P n ) X be a special point not contained in a positive-dimensional special subvariety of X. We show that if a coordinate P i corresponds to an order not contained in a single exceptional Siegel–Tatuzawa imaginary quadratic field K * , then the associated discriminant | Δ ( P i ) | is bounded by an effective constant depending only on deg X and [ 𝔽 : ] . We derive analogous effective results for the positive-dimensional maximal special subvarieties.

From the main theorem we deduce various effective results of André–Oort type. In particular, we define a genericity condition on the leading homogeneous part of a polynomial, and give a fully effective André–Oort statement for hypersurfaces defined by polynomials satisfying this condition.

Funding statement: Gal Binyamini is the incumbent of the Dr. A. Edward Friedmann career development chair in mathematics. This project has received funding from the European Research Council (ERC) under the European Union’s Horizon 2020 research and innovation programme (grant agreement No 802107). This research was supported by the ISRAEL SCIENCE FOUNDATION (grant No. 1167/17) and by funding received from the MINERVA Stiftung with the funds from the BMBF of the Federal Republic of Germany.

A Duke’s theorem avoiding Tatuzawa fields (by Emmanuel Kowalski at Zurich)

Duke’s theorem [9, Theorem 1] for CM points states that as d + , the CM points Λ d of discriminant - d become equidistributed in the modular curve Y ( 1 ) , in the quantitative form

| Λ d Ω | | Λ d | = μ ( Ω ) + O ( | d | - δ )

for some δ > 0 depending only on the domain Ω Y ( 1 ) , which is assumed to be convex with piecewise smooth boundary. Here μ is the hyperbolic area measure normalized so that μ ( Y ( 1 ) ) = 1 . The constant δ > 0 and the implied constant depend only on Ω; the former is effective (and explicit), but the latter is not, due to the use of Siegel’s lower bound for class numbers in the proof.

Tatuzawa [28, Theorem 1] has given a form of Siegel’s bound that, for a given ε > 0 , gives an effective (explicit) constant c ( ε ) > 0 (in fact, proportional to ε) such that

| Λ d | > c ( ε ) | d | 1 2 - ε

for all fundamental discriminants d with at most one exception, which may depend on ε. We write d ε * for this exception.

Let F be the standard fundamental domain of SL 2 ( ) . We view Λ d as a subset of F. We consider the regions

Ω R = { z F : 3 2 < Im ( z ) < R } .

Note a minor issue even in a direct application of Duke’s theorem, without consideration of effectivity: this region is not convex in the hyperbolic sense.

The following is however a simple deduction from the principles of the proof, combined with Tatuzawa’s theorem.

Proposition 9.

Let 0 < ε < 1 16 be fixed. Let d ε * be the corresponding exceptional discriminant. Let m 1 be an integer. There exists an effective constant c ( m , ε ) > 0 such that for d > c ( m , ε ) and for d d ε * , we have

1 | Λ d | | { z Λ d : z Ω 8 m } | 1 - 1 4 m .

Remark 10.

(1) The choice R = 8 m is to have the hyperbolic area of Ω R equal to 1 - 1 R .

(2) We sketch the proof with fundamental discriminants, but proceeding as in [7], it extends to all discriminants.

Sketch of proof.

Recall that

| Λ d | = 1 2 π w d | d | 1 2 L ( 1 , χ d ) ,

where w d is the number of roots of unity in the quadratic field with discriminant d, by Dirichlet’s Class Number Formula (see, e.g., [16, (22.59)]).

Let R = 8 m . Consider a smooth compactly supported function ψ : Y ( 1 ) which satisfies 0 ψ 1 , is equal to 1 for z F with imaginary part R 2 (hence on Ω R / 2 ) and vanishes for z with imaginary part R , and such that the partial derivatives of ψ are bounded (by constants depending only on the order of the derivative).

Note that the choice of such a function depends on m. Observe that

1 | Λ d | | { z Λ d : z Ω R } | 1 | Λ d | z Λ d ψ ( z ) .

Now by the spectral decomposition in L 2 ( Y ( 1 ) ) (see, e.g., [15, Theorem 4.7, Theorem 7.3]), we have

ψ ( z ) = μ ψ + 0 + ψ , E ( , 1 2 + i t ) E ( z , 1 2 + i t ) 𝑑 t + j ψ , u j u j ( z ) ,

where

μ ψ = F ψ ( z ) 𝑑 μ ( z ) ,

the functions E ( z , s ) are the Eisenstein series for SL 2 ( ) and ( u j ) runs over an orthonormal basis of the cuspidal subspace of L 2 ( Y ( 1 ) ) , which we may assume consists of Hecke eigenforms.

We have

μ ψ μ ( Ω R / 2 ) = 1 - 2 R ,

hence

1 | Λ d | z Λ d ψ ( z ) 1 - 1 4 m + ,

where

= 0 + ψ , E ( , 1 2 + i t ) 1 | Λ d | z Λ d E ( z , 1 2 + i t ) d t + j ψ , u j 1 | Λ d | z Λ d u j ( z ) .

A classical formula (see references in [9, p. 88] or [16, (22.45)]) computes

1 | Λ d | z Λ d E ( z , 1 2 + i t ) = w d ζ ( 1 2 + i t ) L ( χ d , 1 2 + i t ) | d | 1 4 - i t 2 L ( 1 , χ d ) ,

where w d is the number of roots of unity in the quadratic field. Combining an old result of Weyl for ζ ( s ) and a result of Heath-Brown [14], whose proof is effective, yields upper bounds

ζ ( 1 2 + i t ) ( 1 + | t | ) 1 6 , L ( χ d , 1 2 + i t ) | d | 1 6 + η ( 1 + | t | ) 1 6 + η

for any η > 0 , where the implied constant is effective and depends only on η.

On the other hand, using the Waldspurger formula (see the discussion of Michel and Venkatesh [21, (2.5)]), one finds a formula of the (similar) type

| 1 | Λ d | z Λ d u j ( z ) | 2 = α L ( u j , 1 2 ) L ( u j × χ d , 1 2 ) | d | 1 2 L ( 1 , χ d ) 2

(where α is a constant) in terms of central values of twisted L-functions. We use the subconvexity estimate of Blomer and Harcos [5, Theorem 2] (although we could use also that of Michel and Venkatesh [22], or indeed any subconvex bound that has polynomial control in terms of the eigenvalue of u j would suffice, and there are many more versions): we have

L ( u j × χ d , 1 2 ) | d | 3 8 ( 1 + | t j | ) 3 , L ( u j , 1 2 ) ( 1 + | t j | ) 3 ,

where the implied constants are effective and 1 4 + t j 2 is the Laplace eigenvalue of the cusp form u j (we have t j since it is known that there are no eigenvalues < 1 4 for Y ( 1 ) ).

Using “integration by parts”, namely writing

ψ , u j = 1 ( 1 4 + t j 2 ) A ψ , Δ A u j = 1 ( 1 4 + t j 2 ) A Δ A ψ , u j ,

we obtain for any A 1 the bound

| ψ , u j | 1 ( 1 4 + t j 2 ) A Δ A ψ A R 2 A + 1 ( 1 + | t j | ) 2 A

(since Δ A ψ ( z ) vanishes unless R 2 Im ( z ) R , and the derivatives are bounded). Similarly, one gets

ψ , E ( , 1 2 + i t ) R 2 A + 1 ( 1 + | t | ) 2 A

for any A > 0 , where the implied constant depends on A and is effective.

Taking A fixed and large enough to make the integral and series converge absolutely (e.g., A = 3 ), we derive the lower bound

1 | Λ d | | { z Λ d : z Ω 8 m } | 1 - 2 R + O ( R 2 A + 1 | d | 1 2 - 1 16 | Λ d | - 1 ) ,

where the implied constant is effective, and hence for d d ε * , we obtain

1 | Λ d | | { z Λ d : z Ω R } | 1 - 2 R + O ( R 2 A + 1 | d | ε - 1 16 ) ,

where the implied constant is effective. The result now follows. ∎

Acknowledgements

I would like to express my gratitude to Jonathan Pila for discussions regarding effectivity issues surrounding André–Oort, and in particular for pointing me in the direction of Tatuzawa’s result; to Elon Lindenstrauss for suggesting Duke’s equidistribution result as a potential remedy for the compactness condition in my paper [4]; and to Gabriel Dill and the anonymous referee for some corrections and suggestions on the initial version of the manuscript. I also thank the Tokyo Institute of Technology for their hospitality during a visit in which some of this work was carried out.

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Received: 2018-10-09
Revised: 2019-05-15
Published Online: 2019-09-11
Published in Print: 2020-10-01

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