Let p,q,t∈C satisfy M<∣t∣n+1<1. For fixed w∈Tn, let Cw be a contour inside the annulus
A={z∈C∣∣t∣−ϵ<∣z∣<∣t∣−1+ϵ}
for infinitesimally small positive ϵ, with the points t−1wj for j∈{1,…,n+1} in its interior, and put Cwn=Cw×⋯×Cw. Let f be a Cn-symmetric function holomorphic on An, and let x∈Cn satisfy ∣t∣<∣xj∣<∣t∣−1. Here κA and κC are the normalization factors and Δ(C,A) is the kernel displayed in the source. (C,A) inversion formula. One has
κAκC∫Tn(∫CwnΔ(C,A)(z,w,x;t)f(z)zdz)wdw=f(x),
where
Δ(C,A)(z,w,x;t)=∏i=1nΓ(zi±2)∏1≤i<j≤nΓ(zi±zj±)∏i=1n∏j=1n+1Γ(txi±wj−1,t−1zi±wj)×∏1≤i<j≤n+1Γ(wiwj−1,wi−1wj,t−2wiwj,t2wi−1wj−1)1.
The formula is proposed as a companion to the preceding inversion theorem for elliptic beta integrals; its status is not resolved in the supplied text.