Point-reflect the sky and even multipoles stay put while odd ones flip; an isotropic Gaussian field balances power between the families, and the measured sky prefers odd from ell of 2 to 30 at persistent 2-to-3σ (Kim and Naselsky 2010; Planck confirmed). The preference entangles with the quadrupole deficit and points loosely along the anomaly family's directions, and the model can only buy it as another fluctuation from the same depleted account.
Parity balance is inherited from inflation's initial conditions: a Gaussian field with no center and no handedness cannot prefer either family. The model has no dial, so the preference must be chance or contamination, verdicts that must also cover the deficit and alignments it interlocks with.
SCT's large-scale field has both of the things point parity cannot survive: a finite deposition domain and an orientation. Perturbations laid down within a bounded overlap volume (P26, P55) populate modes relative to that domain's geometry rather than an infinite centerless ensemble, and a bounded, oriented deposit generically feeds the antisymmetric family differently from the symmetric one, odd-mode preference and even-mode (quadrupole) suppression arriving as two ends of one spectral reshaping. The registered unified treatment prices the family together, the suppressed quadrupole at a quarter of expectation, the hemispheric amplitude at 1.07, the parity preference, from the single 29th-level collision event (Paper 11, From Chaos to Covariant Completeness), with the imprint structure laid out in Paper 8, From Chaos To Constructive Relativity.
The accounting asymmetry is the recurring theme of this family: ΛCDM owes a separate 1-in-100 payment for the parity preference, the deficit, the alignment, the modulation, and the phase correlations, while the cascade pays once for the geometry of one event and collects all five signatures. Sub-horizon physics stays exactly standard (P29, P30), which is why the oddity lives only where the deposition's shape can show.
No premises are spent that the family has not already paid for: the boundary and the axis do all the work.
The registered kill is recurrence-with-correlation: polarization parity statistics (LiteBIRD, CMB-S4) finding even-odd balance fully restored, or a parity preference recurring without correlation to the quadrupole suppression and the family axes, would respectively dissolve the signature or break the one-event reading. The unified mechanism specifically requires the parity preference and the quadrupole deficit to be statistically linked, a checkable joint prediction chance does not make.