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89.4

prescription. The target is the independently frozen original-rod lapse on , , with and . The coordinate clock is ; the positive classical lapse is calibrated to , not . The rods are slice harmonic with decaying corrections and no lapse weight. The output density is XX-A's fixed label density; .

GateScope and ending
Q1XX-B: closed only for the stated compact-test gauge-fixed free multiplet, normalized causal inverses, and algebraic Hadamard class.
Q2XX-C: not closed. Local subtraction and compact-source tails are supplied; positive physical state selection and native covariance estimates are not.
Q3XX-D: open. Classical insertion and compact-cutoff symbols are constructed; native one-contraction admission remains conditional. XX-F's weighted criteria are not verification for a selected representative.
Q4XX-E and XX-F: native breaking application and complete quantum remainder remain unentered/unclosed. Theorem thm:release releases comparison and conditional interface results only.
Q5No native quantum operation, evaluated complete breaking, admissible cancellation, or interacting identity. Theorems thm:breaking–thm:repair remain conditional on constructed native data.

qualification and retained controls. The unfiltered central-second-jet obstruction is proved by Theorem thm:unfiltered; it begins at total on the specified weighted regular algebra (Theorem thm:filtered). The free-equation quotient failure still occurs at . Compact residuals remain zero. The subsidiary defect, unverified infrared hypotheses, conditional one-contraction status, two-rod inverse-distance component, pure-trace blind sector, and escaping-source non-determination remain explicit. Section sec:ledger retains every XIX-A/B/C/D/E, XVIII-A/B, Em02-E, XVI-Q, XX-B/C/D/E, OpenAI catalogue, and XIV separation. No comparison is a transferred native construction.

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