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This companion of the Projective Residue Schur reduction (PRS) examines the Lorentzian saturation functional controlling the generation split u. The symmetric square of the J_Π-odd modulus is J_Π-even and cannot carry the orientation sign; the carrier is taken, by hypothesis, to be an odd antisymmetric chiral two-form F_μν(s). B_sat(s) is defined as the Born–Infeld determinantal saturation margin of such a supplied two-form, and its second variation μ_χ² = ½ P_μν P^μν is the Lorentzian genus of the chiral polarisation P. Hypotheses that no source supplies are stated where used: a Lorentzian co-metric, the construction of the two-form, a local-minimum reading of A4, the existence and non-degeneracy of a locked pair, the covariance of the locking family under J_Π, and, from PRS, its generation-reading and first-order transport hypotheses. The scope is that of PRS: under its generation-reading hypothesis the split vanishes for the reference operator, the consequences for a general locking operator are conditional, and no mechanism for a non-zero split is derived; the identification of the compression remainder with the projective endomorphism of Q14 holds only under the symbol identity Π_S D² Π_S* = Lich. The genus is not determined: the central commutator supplies no electric assignment, since the central direction is not temporal in the co-metrics of the corpus and no map from the generation operator to a two-form is available. The quartic coefficient of the radicand depends on the parametrisation and selects no lock; for a collinear purely electric ray the bound is reached at t* = β/|E|. A conditional factorisation of the contact split to first order in s* (Front D) is given under [H-Gen], [H-Mult], [H-Tr], [H-F], [H-Nd] and the JΠ-covariance and diagonal-form premises of Lemma lem:u-odd, and a localisation hypothesis that fails in the available witnesses of the eliminated-block note, which also fall outside [H-Gen](i); no frame satisfying all these hypotheses together is exhibited, and the factorisation is formal; it fixes no magnitude. The magnitude |u| is not predicted.
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Jérôme Beau (2026) studied this question.
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