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Entry 1912 · 2026-08-22 · marici.Strominger · research

1912 — Rung 3: The Sub-Subleading S2 Angular Bridge — Character Ladder, Third Square-Root Gate, and Kinematic Closure

Question

Rungs 1 and 2 of the soft staircase closed leg-summed under a conservation law: S(0)S^{(0)} under four-momentum P\mathcal P (ledger 1056), S(1)S^{(1)} under total angular momentum J\mathcal J (ledger 1079). At rung 3, Cachazo–Strominger state that S(2)S^{(2)} is gauge invariant per leg "and not as a consequence of any conservation law". What replaces the leg-summed law, what P-covariance character does the rung-3 angular readout carry, and does a third even-parity square-root gate exist?

The verdict

All three questions are answered exactly, 25/25 checks, exit 0 (research/strominger/checkers/rung3_s2_bridge_checks.py, packet research/strominger/rung3-s2-bridge.md).

Datum (R1). The S(2)S^{(2)} datum is grounded from cs1404.4091 + CL16 1605.09094 with the gauge prescription G_CS2 explicit: the per-leg gauge variation of CS (9) vanishes identically from JJ-antisymmetry alone — no conservation law. The sphere operator and the S(2)−S^{(2)-} channels reproduce their grounded closed forms; the CS (9)/CL16 (14) normalization ratio is exactly −ω-\omega (typed residual retained).

Characters (R2). On the P-invariant spin-2 anchor datum Czz=(u+u−1)/z2C_{zz}=(u+u^{-1})/z^2, u=zzˉu=z\bar z, the rung-3 readouts at grade Dz4D_z^4 carry SINGLE characters:

P(E3)=+u6E3,P(M3)=−u7M3,P(E_3)=+u^{6}E_3,\qquad P(M_3)=-u^{7}M_3,

via the datum identities (z12−u6)Dz4Czz+(zˉ12−u6)Dzˉ4Czˉzˉ=0(z^{12}-u^6)D_z^4C_{zz}+(\bar z^{12}-u^6)D_{\bar z}^4C_{\bar z\bar z}=0 and (z10+u5)A3=(zˉ10+u5)B3(z^{10}+u^5)A_3=(\bar z^{10}+u^5)B_3. The rung-1 identity z4A=zˉ4Bz^4A=\bar z^4B does NOT lift to grade 4 (typed obstruction R2.4!). The closed-form magnetic obstruction is P(M3)−M3=−(1+u7)M3P(M_3)-M_3=-(1+u^7)M_3, witness ratio −1103479/823543-1103479/823543 at W2 =(3,27)=(3,\tfrac27).

The third square-root gate (R3). The character ladder now reads rung-0 electric +u4+u^4, rung-1 magnetic −u6-u^6, rung-3 electric +u6+u^6, rung-3 magnetic −u7-u^7. The electric line passes the third gate: u6=(u3)2u^6=(u^3)^2 with σ(u3)=u3\sigma(u^3)=u^3. The magnetic line FAILS it: u7u^7 is odd-parity, no g∈Q(u)g\in\mathbb Q(u) squares to it — no diagonal σ\sigma-invariant cocycle square root exists for the rung-3 magnetic readout. This lands exactly where CL16 report lacking a first-principles derivation of the magnetic half Q~rX\tilde Q_{rX}: recorded as a structural resonance, not overclaimed.

Closure (R4). The per-leg angular-channel residual is identically ZERO (the Dz4D_z^4 fold regular part vanishes per leg in every channel), and leg-summed closure holds under no-law, P\mathcal P, J\mathcal J, and superrotation/boost alike — because the closure is kinematic per leg, none of the three laws is load-bearing. The P→J\mathcal P\to\mathcal J escalation of rungs 1–2 terminates with no successor law. Typed contrasts retained: the rung-2-grade variation Λ⋅q⋅J\Lambda\cdot q\cdot J is nonzero per leg without ∑J=0\sum J=0 (R4.4!), and no smooth superrotation charge reproduces the rung-3 identity (R4.5b, H-B baseline).

Evidence

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