Sharp whole-horizon low-order propagation for the actual child fields. On good times only the negative part of f' can increase the upper pressure bound; history and early times use the exponentially small target ratio. No child low bound is assumed.
The exact source (20) errors, expressed on the same normalized packet that defines the physical child. These are precisely the two errors supplied by the same-Q packet choice.
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The literal strict errors returned by the global same-Q packet theorem imply the error record without any additional analytic bound.
The full horizon has one fixed absolute-size cost, while the upper pressure cost retains delta on good times and the exponentially small bad-time ratio. The parent constants remain the actual sharp CM and CH.