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Self-Dual Holomorphic Cusp Form Rigidity

Updated 8 December 2025
  • Self-dual holomorphic cusp forms are normalized newforms with trivial or quadratic nebentypus that ensure all Fourier coefficients are real.
  • The principal theorem proves that the eventual sign patterns of Fourier coefficients uniquely determine the form up to scaling under precise level and weight conditions.
  • The study employs analytic methods such as Rankin–Selberg convolution, Sato–Tate equidistribution, and Ramakrishnan’s lift, highlighting its impact on modular forms and L-function theory.

A self-dual holomorphic cusp form is a normalized newform fSknew(Γ0(M))f \in S_k^{\mathrm{new}}(\Gamma_0(M)), lying in the space of weight-kk holomorphic cusp forms on Γ0(M)\Gamma_0(M) (a congruence subgroup of SL2(Z)\mathrm{SL}_2(\mathbb{Z})), with trivial or quadratic nebentypus, for which the associated automorphic representation πf\pi_f of GL2(AQ)\mathrm{GL}_2(\mathbb{A}_\mathbb{Q}) is isomorphic to its contragredient. This self-duality condition equivalently asserts that the central character ωf\omega_f of πf\pi_f satisfies ωf2=1\omega_f^2=1, thus ωf\omega_f is at most quadratic and all Fourier coefficients af(n)a_f(n) are real for all nn.

1. Formal Definition and Context

Given integers M1M \geq 1 and k2k \geq 2, the space Sk(Γ0(M))S_k(\Gamma_0(M)) consists of holomorphic cusp forms of weight kk and level MM. Its subspace Sknew(Γ0(M))S_k^{\mathrm{new}}(\Gamma_0(M)) comprises newforms, that is, primitive Hecke eigenforms. For f(z)=n1af(n)e2πinzf(z) = \sum_{n \geq 1} a_f(n) e^{2\pi i n z}, af(n)Ca_f(n) \in \mathbb{C}, self-duality of ff is equivalent to πfπf\pi_f \simeq \pi_f^\vee or, in terms of nebentypus, ωf2=1\omega_f^2=1. Forms with trivial or quadratic nebentypus therefore satisfy self-duality, and in this case all af(n)a_f(n) are real. Self-dual holomorphic cusp forms play a foundational role in the arithmetic theory of modular forms and the analytic study of automorphic LL-functions and representations (Booker, 5 Dec 2025).

2. Principal Theorem: Determination by Sign Patterns

Let fSknew(Γ0(M))f \in S_k^{\mathrm{new}}(\Gamma_0(M)) and gSnew(Γ0(N))g \in S_\ell^{\mathrm{new}}(\Gamma_0(N)) be nonzero normalized newforms with af(n),ag(n)Ra_f(n), a_g(n) \in \mathbb{R}. The principal result, proven by Booker, establishes a rigidity phenomenon for self-dual holomorphic cusp forms under sign conditions:

Theorem (Booker):

Suppose M,N1M, N \geq 1 are such that lcm(M,N)\mathrm{lcm}(M, N) is not divisible by 242^4 nor by the square of any odd prime. Then, the following are equivalent:

  1. af(n)ag(n)0a_f(n)a_g(n) \geq 0 for all sufficiently large nNn \in \mathbb{N}.
  2. (M,k)=(N,)(M, k) = (N, \ell) and f(z)=cg(z)f(z) = c g(z) for some c>0c > 0.

Consequently, if ff and gg are not proportional, then both sets {nN:af(n)ag(n)>0}\{ n \in \mathbb{N} : a_f(n)a_g(n) > 0 \} and {nN:af(n)ag(n)<0}\{ n \in \mathbb{N} : a_f(n)a_g(n) < 0 \} are infinite. This result demonstrates that—under mild, explicit conditions on the level—a self-dual newform is determined up to scaling by the eventual signs of its Fourier coefficients (Booker, 5 Dec 2025).

3. Hypotheses and Technical Conditions

Three technical conditions underlie the theorem:

  • Newform and Non-CM Condition: Both forms ff and gg must be newforms (primitive Hecke eigenforms) and must not admit complex multiplication (CM), ensuring applicability of Rankin–Selberg and Sato–Tate methods.
  • Level Restriction: lcm(M,N)\mathrm{lcm}(M, N) must not be divisible by 242^4 or by the square of any odd prime, excluding certain twist-minimal pathologies (see Remark (1) in (Booker, 5 Dec 2025)).
  • Sign Assumption: There exists N0N_0 such that af(n)ag(n)0a_f(n)a_g(n) \geq 0 for all nN0n \geq N_0 (eventual nonnegativity). In fact, the required assumption can be weakened to hold only along an arithmetic progression of positive density.

These conditions are necessary for both the analytic arguments and the rigidity conclusions; the level constraint is sharp, as explicit counterexamples can be constructed with quadratic twists otherwise.

4. Proof Strategy and Analytical Framework

The proof bifurcates depending on equality of weights/levels:

Case A: (M,k)(N,)(M, k) \neq (N, \ell)

If af(n)ag(n)0a_f(n)a_g(n) \geq 0 for a set of primes pp of Dirichlet density near $1$, the Rankin–Selberg LL-series attached to ff and gg produces analytic contradictions. The analysis is founded on:

  • Hecke eigenbases decompositions of ff and gg into non-CM, twist-minimal newforms,
  • Ramakrishnan's lift from GL2×GL2\mathrm{GL}_2 \times \mathrm{GL}_2 to GL4\mathrm{GL}_4, providing distinct automorphic representations,
  • Rankin–Selberg estimates: pxλf(p)λg(p)/p=O(1)\sum_{p \leq x} \lambda_f(p)\lambda_g(p)/p = O(1) and px(λf(p)λg(p))2/p=Cpx1/p+O(1)\sum_{p \leq x} (\lambda_f(p)\lambda_g(p))^2/p = C \sum_{p \leq x} 1/p + O(1) for C>0C>0,
  • Application of Cauchy–Schwarz and Deligne's bounds to derive a contradiction from the sign constraint.

Case B: (M,k)=(N,)(M, k) = (N, \ell)

Here, ff and gg reside in the same newform space of dimension d1d\geq1. The key innovation is a "dense sign-pattern" argument:

  • By joint Sato–Tate equidistribution, for any two non-CM, twist-inequivalent newforms, the vector of signs of their Fourier coefficients at powers of suitable primes becomes dense in projective space RPd1\mathbb{RP}^{d-1},
  • This density allows, via linear-algebraic separation of the coefficient vectors, the explicit construction of nn where af(n)a_f(n) and ag(n)a_g(n) differ in sign, unless ff and gg are proportional,
  • Overall, eventual agreement of sign patterns enforces proportionality.

5. Examples, Corollaries, and Level Sharpness

  • For distinct non-CM normalized newforms f,gf, g of the same weight and level, both the sets where af(n)ag(n)>0a_f(n)a_g(n) > 0 and af(n)ag(n)<0a_f(n)a_g(n) < 0 are infinite.
  • If f,gf, g differ in weight or level, the same conclusion holds if af(p)ag(p)0a_f(p)a_g(p) \geq 0 for almost all primes pp.
  • The level condition is optimal: If Δ\Delta divides MM to square-power, it is possible to construct g=2f+f(Δ)g = 2f + f \otimes \left( \frac{\Delta}{\cdot} \right) so af(n)ag(n)0a_f(n)a_g(n) \geq 0 for all nn, even though gcfg \neq c f for any scalar cc.
  • No effective bound exists for the first sign difference between ff and gg when the newspace is multidimensional, as gεfg_\varepsilon \to f allows the first disagreement to be arbitrarily delayed.

6. Significance and Connections to Automorphic Theory

The determination of self-dual holomorphic cusp forms by sign patterns of their Fourier coefficients provides a sharp analogue to "multiplicity one" phenomena in representation theory: the sign-sequence captures all information about the form up to scaling. The proof leverages deep arithmetic and analytic properties—most notably Deligne's bounds, functoriality via Ramakrishnan’s transfer, Rankin–Selberg convolution theory, and equidistribution results of Sato–Tate for joint eigenangles (contributions of Barnet-Lamb, Gee, Geraghty, and Wong). The density-and-linear-algebra method introduced for the equal-weight case offers potential applications to other sign-rigidity questions in automorphic forms.

The result addresses outstanding questions on sign changes of Fourier coefficients, complementing previous works (KLSW, Matomäki, GKR) by demonstrating that, in the generic (non-pathological) setting, the sign pattern not only oscillates but characterizes the form itself (Booker, 5 Dec 2025).

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