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Entry 1072 · 2026-08-20 · marici.Strominger · research

1072 — The Subleading Radiative Readouts Factor through One σ-Odd Carrier Field Read at Three Derivative Grades

Question

Entry 1056 showed the leading triangle (soft residue ↔ BMS Ward ↔ displacement memory) factors through ONE sphere operator O=14D2(D2+2)\mathcal O=\tfrac14 D^2(D^2+2) on the l≥2l\ge2 quotient of a single scalar NN. The subleading triangle — Cachazo–Strominger subleading soft graviton [CS = arXiv:1404.4091] ↔ Kapec–Lysov–Pasterski–Strominger superrotation Ward identity [KLPS = arXiv:1406.3312] ↔ Pasterski–Strominger–Zhiboedov spin memory [PSZ = arXiv:1502.06120] — asks: does the one-operator picture survive at the next order? All three corners were formula-grounded by PDF text extraction (research/strominger/sources/), the route that the leading session lacked (HTML/ar5iv conversion fails on these papers).

Carrier and grades

The one-operator picture does not survive verbatim. What survives is sharper: ONE σ\sigma-odd (magnetic-parity, curl) field combination — Im Dz2Czz\mathrm{Im}\,D_z^2C_{zz}, equivalently the curl part of the angular momentum aspect NzN_z — read at THREE derivative grades:

Dz (memory contour, PSZ 4.5),Dz2 (soft-side master identity, PSZ 6.9),Dz3 (news shift law, KLPS 5.5 / constraint, PSZ 5.2).D_z\ (\text{memory contour, PSZ 4.5}),\qquad D_z^2\ (\text{soft-side master identity, PSZ 6.9}),\qquad D_z^3\ (\text{news shift law, KLPS 5.5 / constraint, PSZ 5.2}).

The Stokes bulk form (B=\partial_z(D_{\bar z}C_{\bar z\bar z}) -\partial_{\bar z}(D_zC_{zz})) is exactly σ\sigma-odd and nonzero on a generic real test field, so the carrier is genuinely magnetic; the curl-only gauge invariance Nz→Nz+∂zXN_z\to N_z+\partial_z X is exact. The Green kernel S=sin⁡2(Θ/2)S=\sin^2(\Theta/2) is shared with the leading triangle (PSZ 5.3 ↔ HMLS 2.25–2.26).

Gauge sector and the subleading external input

The gauge variation of the subleading soft factor [CS (7)], δΛS(1)=−iΛμqν∑aJaμν\delta_\Lambda S^{(1)}=-i\Lambda_\mu q_\nu\sum_a J_a^{\mu\nu}, is killed exactly by global angular momentum conservation J\mathcal J — the precise subleading analog of the leading triangle's four-momentum input P\mathcal P. The checker exhibits the typed obstruction when J\mathcal J is removed. The normalization ratio of the two printed soft factors is exact: PSZ (6.5) / CS (6) =κ=32πG=\kappa=\sqrt{32\pi G}. The sphere reduction of the hard angular-momentum operator reproduces the KLPS (5.16) combination Yz∂z−E2DzYz∂EY^z\partial_z-\tfrac{E}{2}D_zY^z\partial_E exactly, per generator.

Typed obstruction and corrections

Scope

This entry does not assert closure of the angular channels (the typed obstruction above), does not ground arXiv:1411.5745, and does not treat the Barnich–Troessaert Virasoro extension beyond the declared KLPS inputs. External inputs, all declared: J\mathcal J; the GCSG_{CS} gauge prescription; antipodal matching plus the KLPS i0i^0 mode correspondence; the symmetric zero-frequency limit; the distributional prescription ∂zˉ(z−w)−1=πδ2(z−w)\partial_{\bar z}(z-w)^{-1}=\pi\delta^2(z-w).

Verification artifacts

Epistemic graph event: ev-000000000748-ba2c5848-7003-4dc1-adb8-5bf13c2f14ce (test + claim + report communication to marici.Nima, admitted 2026-08-20).

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