Serre (1997) proved that the eigenvalues of the normalized Hecke operator Tp′=Tp/p(k−1)/2T_p' = T_p/p^{(k-1)/2} on the space Sk(Γ0(N))S_k(\Gamma_0(N)) of cusp forms equidistribute in [−2,2][-2,2] with respect to the pp-adic Plancherel measure μp\mu_p as k+N→∞k+N\to\infty over levels prime to pp, and deduced two arithmetic consequences for the number fields KiK_i generated by Hecke eigenvalues: for fixed weight kk and fixed r≥1r\ge1, the proportion s(N,k)r/s(N,k)s(N,k)_r/s(N,k) of eigenforms whose Hecke field has degree exactly rr tends to 00 along levels coprime to any fixed prime (Theorem 5), and the maximal degree r(N,k)r(N,k) tends to ∞\infty with NN (Theorem 6, proved using oldforms). He asked what happens outside this regime: whether the coprimality hypothesis can be dropped; what happens at fixed level NN as the weight k→∞k\to\infty; whether the decay is a power saving s(N,k)r≪s(N,k)αs(N,k)_r \ll s(N,k)^\alpha with α<1\alpha<1; and the newform version of Theorem 6. The later literature resolves the newform version in the main (Royer; Murty–Sinha; Bettin–Perret-Gentil–Radziwiłł: the largest simple Hecke submodule of the new subspace has dimension ≫klog⁡log⁡N/log⁡(2pN)\gg_k \log\log N/\log(2p_N) for every NN) and gives exponential-in-(log⁡N)β(\log N)^\beta multiplicity bounds at prime level, extended by Sarnak–Zubrilina to composite levels that are not ‘super-smooth’ (their §6, Theorem 5) while explicitly excluding primorial-type levels, and stated by them to fall short of Serre's conjectural power saving. The weight aspect at fixed level is bounded below only in Galois-orbit counts (Dieulefait–Pacetti–Tsaknias; Banerjee et al.) and is governed by the still-open Maeda conjecture and its generalizations, and has recent heuristic support at squarefree level for weight 2 (Cowan–Martin). The surviving open core is: (1) the proportion limit over all levels, including levels divisible by every small prime; (2) unboundedness of maximal Hecke-field degree at fixed level, open already at level 1; (3) power-saving bounds for general weight and degree.

Background

For N≥1N\ge1 and even k≥2k\ge2, let Sk(Γ0(N))S_k(\Gamma_0(N)) denote the complex vector space of holomorphic cusp forms of weight kk for the congruence subgroup Γ0(N)\Gamma_0(N) of SL2(Z)\mathrm{SL}_2(\mathbb{Z}), i.e. matrices (abcd)\begin{pmatrix}a&b\\c&d\end{pmatrix} with integer entries and c≡0(modN)c\equiv0\pmod{N}; write s(N,k)=dim⁡Sk(Γ0(N))s(N,k)=\dim S_k(\Gamma_0(N)). A cusp form is a holomorphic function on the upper half-plane satisfying the weight-kk transformation law under Γ0(N)\Gamma_0(N) and vanishing at the cusps; its Fourier expansion f=∑m≥1a(m)qmf=\sum_{m\ge1}a(m)q^m (with q=e2πizq=e^{2\pi iz}) determines it. For a prime ℓ∤N\ell\nmid N, the Hecke operator TℓT_\ell acts by Tℓf=∑m≥1(a(ℓm)+ℓk−1a(m/ℓ))qmT_\ell f=\sum_{m\ge1}(a(\ell m)+\ell^{k-1}a(m/\ell))q^m, where a(x)=0a(x)=0 unless xx is a positive integer; the operators TnT_n with (n,N)=1(n,N)=1 commute and are simultaneously diagonalizable, so there is a basis f1,…,fs(N,k)f_1,\dots,f_{s(N,k)} with Tnfi=xi,nfiT_n f_i=x_{i,n}f_i. The eigenvalues xi,nx_{i,n} are totally real algebraic integers, and the field Ki=Q(xi,n:(n,N)=1)K_i=\mathbb{Q}(x_{i,n}:(n,N)=1) is the Hecke field of fif_i; Serre writes s(N,k)rs(N,k)_r for the number of indices ii with [Ki:Q]=r[K_i:\mathbb{Q}]=r, so ∑r≥1s(N,k)r=s(N,k)\sum_{r\ge1}s(N,k)_r=s(N,k), and r(N,k)r(N,k) for the maximal degree [Ki:Q][K_i:\mathbb{Q}].

By the Ramanujan conjecture (proved by Deligne), the eigenvalues of the normalized operator Tp′=Tp/p(k−1)/2T_p'=T_p/p^{(k-1)/2} lie in [−2,2][-2,2]. Serre's Theorem 1 (1997) states that for any sequence of pairs (kλ,Nλ)(k_\lambda,N_\lambda) with kλk_\lambda even, kλ+Nλ→∞k_\lambda+N_\lambda\to\infty, and p∤Nλp\nmid N_\lambda, these eigenvalues equidistribute in [−2,2][-2,2] for the measure

μp=p+1π⋅(1−x2/4)1/2(p+1/p)2−x2 dx,\mu_p=\frac{p+1}{\pi}\cdot\frac{(1-x^2/4)^{1/2}}{(\sqrt p+1/\sqrt p)^2-x^2}\,dx,

the pp-adic Plancherel measure (the pushforward of normalized Haar measure on SL2(Zp)\mathrm{SL}_2(\mathbb{Z}_p) under the trace map), which is not the classical Sato–Tate measure 1π(1−x2/4)1/2dx\frac{1}{\pi}(1-x^2/4)^{1/2}dx and had earlier appeared in the spectral theory of arithmetic graphs. The proof uses the Eichler–Selberg trace formula for the traces of Hecke operators on Sk(Γ0(N))S_k(\Gamma_0(N)).

Atkin–Lehner theory decomposes Sk(Γ0(N))S_k(\Gamma_0(N)) into an old subspace (spanned by forms of lower level and their level-raising copies) and a new subspace Sk(Γ0(N))newS_k(\Gamma_0(N))^{\mathrm{new}} spanned by newforms, i.e. normalized eigenforms not coming from lower level. The Galois conjugates σ(f)\sigma(f), σ∈Gal(Q‾/Q)\sigma\in\mathrm{Gal}(\overline{\mathbb{Q}}/\mathbb{Q}), of a newform are again newforms of the same level with conjugate eigenvalues, so the Galois orbit of ff has exactly [Kf:Q][K_f:\mathbb{Q}] elements; equivalently, the Q\mathbb{Q}-algebra generated by the Hecke operators decomposes into simple factors whose Q\mathbb{Q}-dimensions are these degrees. In weight 2, Shimura (with later refinements by Ribet) identifies these factors with the Q\mathbb{Q}-simple factors of the Jacobian J0(N)J_0(N) of the modular curve X0(N)X_0(N): if J0(N)∼∏jAjJ_0(N)\sim\prod_j A_j is the decomposition up to Q\mathbb{Q}-isogeny, then Q⊗End(Aj)\mathbb{Q}\otimes\mathrm{End}(A_j) is a totally real field EjE_j with [Ej:Q]=dim⁡Aj[E_j:\mathbb{Q}]=\dim A_j, and the multiset of Hecke fields KiK_i is the multiset of real embeddings of the EjE_j; in particular s(2,N)r/rs(2,N)_r/r counts the Q\mathbb{Q}-simple factors of J0(N)J_0(N) of dimension rr.

From his equidistribution theorem Serre deduced, for fixed weight kk: Theorem 5, that for every fixed prime pp and every r≥1r\ge1, s(N,k)r/s(N,k)→0s(N,k)_r/s(N,k)\to0 as N→∞N\to\infty through levels prime to pp (in his words, most Hecke fields have large degree); Theorem 6, that r(N,k)→∞r(N,k)\to\infty as N→∞N\to\infty, with no coprimality hypothesis, but proved by passing to oldforms; and Theorem 7, that the largest dimension of a Q\mathbb{Q}-simple factor of J0(N)J_0(N) tends to ∞\infty with NN. He then asked what happens outside this regime, in four recorded directions: (i) can the hypothesis that NN is prime to the fixed prime pp be removed in Theorem 5 ("Cela paraît vraisemblable, mais je ne sais pas le démontrer.")? (ii) what happens when the level NN is fixed and the weight kk varies ("J'ignore ce qui se passe lorsque l'on fixe NN et fait varier kk.")? (iii) is the decay a power saving, s(N,k)r/Nα→0s(N,k)_r/N^\alpha\to0 for some α<1\alpha<1, or even for every α>0\alpha>0? (iv) Theorem 5 also holds for the new subspace, but "J'ignore ce qu'il en est du th. 6", since that proof uses oldforms. In the weight aspect at level 1, Maeda's conjecture (recorded by Hida and Maeda in 1997) predicts far more than unboundedness: for every even kk, the space Sk(Γ0(1))S_k(\Gamma_0(1)) is a single Galois orbit, i.e. one Hecke field of maximal degree dim⁡Sk(Γ0(1))\dim S_k(\Gamma_0(1)). For the fixed-level weight aspect, an orbit count gives a sufficient condition: r(N,k)→∞r(N,k)\to\infty follows if the number of Galois orbits of eigenforms in Sk(Γ0(N))S_k(\Gamma_0(N)) is o(dim⁡Sk(Γ0(N)))o(\dim S_k(\Gamma_0(N))) as k→∞k\to\infty.

Problem Statement

Fix an even weight k≥2k\ge2 and a level N≥1N\ge1, and keep the notation of Serre (1997): Sk(Γ0(N))S_k(\Gamma_0(N)) is the space of cusp forms for Γ0(N)\Gamma_0(N), TnT_n (for nn prime to NN) the Hecke operators, f1,…,fs(N,k)f_1,\dots,f_{s(N,k)} a simultaneous eigenbasis with Tnfi=xi,nfiT_n f_i=x_{i,n}f_i, Ki=Q(xi,n)K_i=\mathbb{Q}(x_{i,n}) the Hecke fields, s(N,k)r=#{i:[Ki:Q]=r}s(N,k)_r=\#\{i:[K_i:\mathbb{Q}]=r\}, s(N,k)=dim⁡Sk(Γ0(N))s(N,k)=\dim S_k(\Gamma_0(N)), and r(N,k)r(N,k) the maximal degree. Serre's Theorem 5 gives s(N,k)r/s(N,k)→0s(N,k)_r/s(N,k)\to0 as N→∞N\to\infty (for fixed kk, fixed rr) along levels prime to a fixed prime pp, and Theorem 6 gives r(N,k)→∞r(N,k)\to\infty as N→∞N\to\infty (for fixed kk, no coprimality, proved via oldforms). The later literature resolves the newform version of Theorem 6 in the main and quantifies the decay in restricted regimes, leaving the open core of Serre's questions; the three components share one objective — extend the degree-growth theory of Theorems 5–6 over the full (N,k)(N,k)-plane with quantitative control — and components 1 and 3 are linked by the same obstruction (levels divisible by every small prime):

  1. Coprimality (Serre's question after Theorem 5). For fixed kk and every fixed r≥1r\ge1, determine whether s(N,k)r/s(N,k)→0s(N,k)_r/s(N,k)\to0 as N→∞N\to\infty over all positive integers NN, with no coprimality hypothesis. Since the restriction to levels coprime to any fixed prime is Theorem 5 itself, the open content is uniformity over levels divisible by every fixed prime, e.g. primorials; the same regime is where the best unconditional lower bound for the maximal Hecke-field degree of newforms degenerates to an absolute constant.

  2. Weight aspect (Serre's remark after Theorem 6). For fixed level NN — already for N=1N=1 — determine whether r(N,k)→∞r(N,k)\to\infty as k→∞k\to\infty.

  3. Quantitative rate (Serre's second remark in §6.1). For fixed kk and rr, determine whether a power-saving bound holds, i.e. whether s(N,k)r=O(s(N,k)α)s(N,k)_r=O(s(N,k)^\alpha) for some α<1\alpha<1 (the source asks for s(N,k)r/Nα→0s(N,k)_r/N^\alpha\to0 for some α<1\alpha<1, or even for every α>0\alpha>0), without coprimality or primality restrictions on the levels.

Each of the three components is posed independently and is to be settled in the stated generality, i.e. without additional hypotheses — prime level, fixed Atkin–Lehner sign pattern, restricted sets of levels, or a fixed prime excluded from the level.

References

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