Helper lemmas for dimension-one arguments #
In a rank-one module, every element is a scalar multiple of any nonzero element.
Symmetric version: c • e = f instead of f = c • e.
Convert smul equality of modular forms to pointwise equality.
E₄ is 1-periodic: E₄(z + 1) = E₄(z). This follows from E₄ being a modular form for Γ(1).
E₆ is 1-periodic: E₆(z + 1) = E₆(z). This follows from E₆ being a modular form for Γ(1).
E₄ transforms under S as: E₄(-1/z) = z⁴ · E₄(z)
E₆ transforms under S as: E₆(-1/z) = z⁶ · E₆(z)
Equations
- One or more equations did not get rendered due to their size.
Instances For
Imaginary Axis Properties #
Properties of Eisenstein series when restricted to the positive imaginary axis z = I*t.
E_k(it) is real for all t > 0 when k is even and k ≥ 4.
This is the generalized theorem from which E₄_imag_axis_real and E₆_imag_axis_real follow.
Boundedness of E₂ #
Bound on the q-series ∑ n·qⁿ/(1-qⁿ) that appears in E₂.
For ‖q‖ < 1, we have ‖∑ₙ₌₁ n·qⁿ/(1-qⁿ)‖ ≤ ‖q‖/(1-‖q‖)³.
The key estimates are:
- |1-qⁿ| ≥ 1-|q|ⁿ ≥ 1-|q| for n ≥ 1
- |n·qⁿ/(1-qⁿ)| ≤ n·|q|ⁿ/(1-|q|)
- ∑ n·rⁿ = r/(1-r)², so ∑ n·rⁿ/(1-r) = r/(1-r)³
E₂ is bounded at infinity.
Uses E₂_eq: E₂(z) = 1 - 24·Σₙ₌₁ n·qⁿ/(1-qⁿ) where q = exp(2πiz).
For im(z) ≥ 1, |q| ≤ exp(-2π), so by norm_tsum_logDeriv_expo_le,
|E₂| ≤ 1 + 24·exp(-2π)/(1-exp(-2π))³.
E₄ is bounded at infinity (as a modular form).
The product E₂ · E₄ is bounded at infinity.