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TauCeti.NumberTheory.ModularForms.Newforms.AnalyticInvariants

Analytic rank and conductor of a newform #

For a positive-weight newform, its coefficient Dirichlet series has the entire continuation ModularForm.L. This file defines the analytic rank to be the order of vanishing of that continuation at the central point k / 2. The continuation is not identically zero, because its Dirichlet coefficients have first coefficient one. Consequently the order is finite and is faithfully represented by a natural number.

The analytic conductor is stated in the arithmetic s-coordinate. If s_an = s - (k - 1) / 2 is the analytic normalization, its two archimedean parameters are s_an + (k - 1) / 2 and s_an + (k + 1) / 2. Thus

q(f, s) = N (|s_an + (k - 1) / 2| + 3) (|s_an + (k + 1) / 2| + 3).

The constant 3 and this normalization follow Iwaniec--Kowalski, §5.1 and (5.7).

Main definitions #

Main results #

References #

@[simp]
theorem HeckeRing.GL2.Newform.L_ne_zero {N : ℕ} [NeZero N] {k : ℤ} (f : Newform N k) (hk : 0 < k) :

The normalized first coefficient of a newform ensures that its entire L-function is nonzero, and hence that its analytic order is finite.

@[simp]

The analytic order of the entire L-function of a newform is finite at every point.

noncomputable def HeckeRing.GL2.Newform.analyticRank {N : ℕ} [NeZero N] {k : ℤ} (f : Newform N k) (hk : 0 < k) :

The analytic rank of a positive-weight newform is the order of vanishing of its entire L-function at the central point s = k / 2.

Equations
Instances For
    theorem HeckeRing.GL2.Newform.analyticRank_def {N : ℕ} [NeZero N] {k : ℤ} (f : Newform N k) (hk : 0 < k) :

    The defining equation for the analytic rank.

    theorem HeckeRing.GL2.Newform.analyticRank_eq_analyticOrderNatAt {N : ℕ} [NeZero N] {k : ℤ} (f : Newform N k) (hk : 0 < k) {F : ℂ → ℂ} (hF : Differentiable ℂ F) (hFL : ∀ {s : ℂ}, ↑k / 2 + 1 < s.re → F s = LSeries (fun (n : ℕ) => (PowerSeries.coeff n) (UpperHalfPlane.qExpansion 1 ⇑f.toCuspForm)) s) :

    Any entire continuation agreeing with the coefficient Dirichlet series on the known convergence half-plane computes the analytic rank. In particular, the definition is independent of the chosen construction of analytic continuation.

    @[simp]
    theorem HeckeRing.GL2.Newform.analyticRank_eq_zero_iff {N : ℕ} [NeZero N] {k : ℤ} (f : Newform N k) (hk : 0 < k) :
    f.analyticRank hk = 0 ↔ ModularForm.L hk f.toCuspForm (↑k / 2) ≠ 0

    A newform has analytic rank zero exactly when its entire L-function does not vanish at the central point.

    @[simp]
    theorem HeckeRing.GL2.Newform.analyticRank_pos_iff {N : ℕ} [NeZero N] {k : ℤ} (f : Newform N k) (hk : 0 < k) :
    0 < f.analyticRank hk ↔ ModularForm.L hk f.toCuspForm (↑k / 2) = 0

    A newform has positive analytic rank exactly when its entire L-function vanishes at the central point.

    noncomputable def HeckeRing.GL2.Newform.analyticConductorAt {N : ℕ} [NeZero N] {k : ℤ} (_f : Newform N k) (s : ℂ) :

    The analytic conductor of a newform at an arithmetic parameter s.

    Writing s_an = s - (k - 1) / 2, the two norm factors are the archimedean parameters s_an + (k - 1) / 2 and s_an + (k + 1) / 2.

    Equations
    Instances For
      @[simp]
      theorem HeckeRing.GL2.Newform.analyticConductorAt_eq {N : ℕ} [NeZero N] {k : ℤ} (f : Newform N k) (s : ℂ) :
      f.analyticConductorAt s = ↑N * (‖s‖ + 3) * (‖s + 1‖ + 3)

      In the arithmetic s-coordinate, the two archimedean parameters simplify to s and s + 1.

      noncomputable def HeckeRing.GL2.Newform.analyticConductor {N : ℕ} [NeZero N] {k : ℤ} (f : Newform N k) :

      The analytic conductor of a newform is its analytic conductor at the central point s = k / 2.

      Equations
      Instances For

        The defining equation for the central analytic conductor.

        @[simp]
        theorem HeckeRing.GL2.Newform.analyticConductor_eq {N : ℕ} [NeZero N] {k : ℤ} (f : Newform N k) :
        f.analyticConductor = ↑N * (‖↑k / 2‖ + 3) * (‖↑k / 2 + 1‖ + 3)

        The central analytic conductor in the arithmetic coordinate.

        The analytic conductor at every parameter is strictly positive.

        The central analytic conductor is strictly positive.