Established within the stated premises
Cubic spin Cauchy range has three Hardy channels; strong domain remains separate
finding:cubic-spin-cauchy-range-is-three-hardy-with-strong-domain-distinction
On three normalized disks the closed massless half-form Cauchy range is H²(D)^3. At cubic boundary points z-zj~u³ the coefficient is f~u^-1~|s|^-1/3 and |f|²ds~|s|^-2/3 is integrable. A flat outer factor gives dense compatible smooth boundary germs. Intrinsic H1 retains common vertex values, higher norms retain further jets; the constant derivative sends permitted singular ambient traces out ofL2. Equal L2 ranges therefore do not identify strong domains. Tangential B intertwiners alone do not fix global Calderon projections; bulk Dirac/harmonic data must also be transported. Moreover pi_*S0=O(-1)^3 follows from rank3,chi0,H0=0, so direct pushforward differs from old O(-2)+O(-1)^2 anchor.
Scope: Exact analytic result for explicitly conditional massless spin operator and named ambient core. No smooth Calderon theorem for arbitrary graph domains, freely inserted elementary modification, or physical P1 source/time closure. Scalar Hardy coordinates depend on half-form signs; norm and projection are intrinsic.
Required premises and original source excerpts
- Do not identify source types
Observable algebra, OS reflection, state, collar operator, time evolution, carrier connection, family holonomy, and readout are distinct data until an original map relates them.
premise:typed-source-structures - Recovered genus2 cover with retained coefficients
Retain exactly the older three-sheet cover C:w³=(z²-1)/(z²+1), eta=z(1-w³), eta²=1-w⁶, six Weierstrass points p_a=omega^a,q_a=-omega^a, given z base and clock markings. Seek actual flat coefficient lines for existing v117 monodromy, not mere permutation equivalence or an assumed field intertwiner.
premise:recovered-genus-two-cover-with-retained-signed-coefficients - Massless spin trace on original cubic disk pullback
Exactly C:eta²=1-w⁶, z=eta/(1-w³), S0 with S0²=K and H0(S0)=0. Conditionally consider the massless chiral spin operator on three normalized disk components and the compatible smooth ambient trace with half-form boundary norm integral|psi²|. Strong operator closure is not replaced by L2 range. No identification with the actual P1 operator is assumed.
premise:standard-chiral-spin-trace-on-original-cubic-disk-pullback
- experiments/theory-contracts/elliptic-moebius-source-bridge-20261026/source_unification_20261027/analytic/C3-CAUCHY-HARDY-ARROW.txt, lines 1–200
Source SHA256: 3c8c2b55ca3a58469aaaa61be3e2d74b2075cc33d132fef799790fad22c1bdc2
bounded-excerpt · current-at-snapshot
- experiments/theory-contracts/elliptic-moebius-source-bridge-20261026/source_unification_20261027/analytic/C3-CAUCHY-HARDY-ARROW.txt, lines 201–400
Source SHA256: 3c8c2b55ca3a58469aaaa61be3e2d74b2075cc33d132fef799790fad22c1bdc2
bounded-excerpt · current-at-snapshot
- experiments/theory-contracts/elliptic-moebius-source-bridge-20261026/source_unification_20261027/analytic/C3-CAUCHY-HARDY-ARROW.txt, lines 401–401
Source SHA256: 3c8c2b55ca3a58469aaaa61be3e2d74b2075cc33d132fef799790fad22c1bdc2
bounded-excerpt · current-at-snapshot
- experiments/theory-contracts/elliptic-moebius-source-bridge-20261026/source_unification_20261027/review/C3-CAUCHY-HARDY-ARROW-INDEPENDENT-REVIEW.txt, lines 1–179
Source SHA256: f85492023b0fe82a61da8403c606ae466a5821571ac1b44d164796a30eacd68a
bounded-excerpt · current-at-snapshot