The vocabulary of the Hilbert space inequality #
The objects of the source's key proposition, which speaks only of a finite conjugation-invariant multiset of complex numbers and a test function — no zeta function appears.
A multiset is presented by its finite support Z together with a multiplicity function m, so
every sum is written over a finite set with explicit weights. That is what removes the source's
bookkeeping over conjugate pairs: because gz is conjugation-invariant and hz anti-invariant, a
sum over the whole non-real part equals twice a sum over representatives, with no choice of
representatives to make.
The even part of the twisted pair, gz = (fz z + fz (conj z)) / 2.
Equations
- ZetaZeros.gz eta z u = (ZetaZeros.fz eta z u + ZetaZeros.fz eta ((starRingEnd ℂ) z) u) / 2
Instances For
The odd part of the twisted pair, hz = (fz z - fz (conj z)) / (2i).
Equations
- ZetaZeros.hz eta z u = (ZetaZeros.fz eta z u - ZetaZeros.fz eta ((starRingEnd ℂ) z) u) / (2 * Complex.I)
Instances For
A function ℝ → ℂ is symmetric when conjugation acts as reflection: conj (Φ u) = Φ (-u).
The property is preserved by Gram–Schmidt and is what makes the Bessel coefficients real.
Equations
- ZetaZeros.IsSymmetric Φ = ∀ (u : ℝ), (starRingEnd ℂ) (Φ u) = Φ (-u)
Instances For
The two-variable kernel F (u, v) = ∑ z, m z * fz z u * fz z v, the multiset sum written with
explicit multiplicities.
Equations
- ZetaZeros.bigF eta Z m u v = ∑ z ∈ Z, ↑(m z) * ZetaZeros.fz eta z u * ZetaZeros.fz eta z v
Instances For
The even part is conjugation-invariant.