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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