Hardy Polarized Criterion
Abstract
A finite Hardy Hankel block vanishes exactly when its negative-frequency coefficients vanish.
Theorem 1.1 (Finite Hardy Hankel block vanishing criterion).
Proof. Machine-checked in Lean as D5/S3/Weil/Pick/HardyPolarizedCriterion.hardy_polarized_criterion (✓ std3). ∎
Source. Repository-derived.
Commentary.
For a finite truncation, the Hankel block samples the coefficient sequence at i + j + 1, the negative-frequency tail of a Laurent symbol. Its vanishing is therefore equivalent to the vanishing of every sampled tail coefficient.
This is the finite algebraic Hardy statement. The source-level identification of the symbol with a completed-zeta RH family is not assumed here, because that analytic bridge has no owner in the pinned library.
Theorem 1.2 (A negative coefficient witnesses a nonzero Hankel block).
Proof. Machine-checked in Lean as D5/S3/Weil/Pick/HardyPolarizedCriterion.hardy_nonzero_of_negative_coefficient (✓ std3). ∎
Source. Repository-derived.
Commentary.
Any explicitly nonzero sampled negative-frequency coefficient gives a matrix entry that is nonzero, hence constructs a concrete witness against Hankel-block vanishing.
References
- Truth anchor:
D5/S3/Weil/Pick/HardyPolarizedCriterion.hardy_nonzero_of_negative_coefficient - Truth anchor:
D5/S3/Weil/Pick/HardyPolarizedCriterion.hardy_polarized_criterion