the proof notes, §6: fixed local matrices and exact determinant identities.
lowBlockMatrix = [V⁰(u^{i+k} r_L)], highBlockMatrix = [V⁰(u^{i+k} r_H)], M₀ = [V⁰(u^{i+k} r_0)] with
V⁰(u^e) = e B_{e-1}, V⁰((u+m)^{-1}) = 2 H_m^{(3)} and
r_L = u³/((u+1)(u+2)(u+3)(u+4)), r_H = u³/((u+1)(u+2)(u+3)), r_0 = u/((u+1)(u+2)(u+3)(u+4))
(exact rationals of code/local_blocks_453.py and the FIX table of code/prime_edge_crt453.py).
The Hankel entries depend only on i+k; the moment sequences are recorded separately.
V⁰(u^e r_H), e = 0, …, 2.
Instances For
The three-by-three Hankel block formed from the low moments.
Equations
- Zeta32.PrimeEdge.lowBlockMatrix i k = Zeta32.PrimeEdge.lowMoment ⟨↑i + ↑k, ⋯⟩
Instances For
The two-by-two Hankel block formed from the high moments.
Equations
- Zeta32.PrimeEdge.highBlockMatrix i k = Zeta32.PrimeEdge.highMoment ⟨↑i + ↑k, ⋯⟩
Instances For
The four-by-four Hankel block formed from the zero moments.
Equations
- Zeta32.PrimeEdge.M₀ i k = Zeta32.PrimeEdge.zeroMoment ⟨↑i + ↑k, ⋯⟩
Instances For
theorem
Zeta32.PrimeEdge.M_L_eq :
lowBlockMatrix = !![1565 / 648, -15575 / 648, 101261 / 648;
-15575 / 648, 101261 / 648, -545255 / 648;
101261 / 648, -545255 / 648, 2649929 / 648]