5 problems

Consider self-dual Yang–Mills theory on Burns space with gauge group $\operatorname{SO}(8)$, and let the large $N$ chiral algebra be the celestial chiral algebra described in the p…

Let WZW$_4$ plus Mabuchi gravity be the bulk theory on Burns space, and let the large $N$ chiral algebra be the chiral algebra obtained from the compactification…

Let $\widetilde{\mathbb{F}}$ be the Burns-space twistor compactification and let $\overline{\operatorname{SL}}_2(\mathbb{C})$ be the alternative compactification. Consider holograp…

Let the holographic correlators be defined for insertions at points satisfying $z\neq 0,\infty$, and consider the $\operatorname{SU}(2)\times\operatorname{U}(1)$ isometries of Burn…

Compared to known results about celestial holography, the proposal has a dual chiral algebra defined non-perturbatively, meaning at finite bulk coupling $1/\sqrt N$, rather than on…