Three-point higher-order conformal divergence conjecture

Fix i{1,2,3}i\in\{1,2,3\}. Let sZ03\mathbf{s}\in\mathbb{Z}_{\geq 0}^3, si>0s_i>0, ΔjC\Delta_j\in\mathbb{C} for jij\neq i, and let the depth satisfy ti{0,,si1}t_i\in\{0,\ldots,s_i-1\}. For non-negative exponents h1,h2,h3,v1,v2,v3h_1,h_2,h_3,v_1,v_2,v_3, consider the three-point tensor structure built from H12,H23,H13H_{12},H_{23},H_{13} and V1,23,V2,31,V3,12V_{1,23},V_{2,31},V_{3,12}, with the usual powers of P12,P23,P13P_{12},P_{23},P_{13} determined by the dimensions. Three-point higher-order conformal divergence conjecture. There exists a differential operator Di,siti\mathcal{D}_{i,s_i-t_i} acting on C[Hij,Vi,jk]\mathbb{C}[H_{ij},V_{i,jk}] such that

(PiDZi)siti(f(H12h1H23h2H13h3V1,23v1V2,31v2V3,12v3P12τ12,3P23τ23,1P13τ31,2))=f(Di,siti(H12h1H23h2H13h3V1,23v1V2,31v2V3,12v3)P12τ12,3P23τ23,1P13τ31,2),(\partial_{P_i}\cdot D_{Z_i})^{s_i-t_i}\left(f\left(\frac{H^{h_1}_{12}H^{h_2}_{23}H^{h_3}_{13}V^{v_1}_{1,23}V^{v_2}_{2,31}V^{v_3}_{3,12}}{P^{\tau_{12,3}}_{12}P^{\tau_{23,1}}_{23}P^{\tau_{31,2}}_{13}}\right)\right)=f\left(\frac{\mathcal{D}_{i,s_i-t_i}(H^{h_1}_{12}H^{h_2}_{23}H^{h_3}_{13}V^{v_1}_{1,23}V^{v_2}_{2,31}V^{v_3}_{3,12})}{P^{\tau_{12,3}}_{12}P^{\tau_{23,1}}_{23}P^{\tau_{31,2}}_{13}}\right),

if and only if Δi=d1+ti\Delta_i=d-1+t_i, where

v1+h1+h3=s1,v2+h1+h2=s2,v3+h2+h3=s3.v_1+h_1+h_3=s_1,\qquad v_2+h_1+h_2=s_2,\qquad v_3+h_2+h_3=s_3.

This is the proposed three-point extension of the preceding first-order differential-operator theorem.

Sources & referencesView supporting material

Primary source

Viktoriia Borovik, Claire de Korte, Nathan Meurrens and Dmitrii Pavlov, “Constraining Conformal Correlators”, arXiv:2605.31491 (2026).

Progress summary

Never refreshed

Nothing recorded yet. Refresh searches the literature and the public web for attempts on this problem, and writes the first summary here.

Solutions 0

No solutions have been posted yet.