Hidden simplicity in AdS spinning Mellin amplitudes via scaffolding

TL;DR

This paper reveals a surprisingly simple structure in Mellin amplitudes for tree-level AdS holographic correlators involving spinning operators, using scaffolding techniques that generalize flat-space amplitudes and simplify the understanding of these complex objects.

Contribution

It introduces a scaffolding method to construct Mellin amplitudes for spinning operators in AdS, revealing hidden simplicity and matching flat-space amplitude structures.

Findings

Mellin amplitudes for spinning operators can be constructed from scalar scaffolding.

Vertices with descendant levels are proportional to primary vertices with combinatorial coefficients.

The results exhibit a simple form analogous to flat-space amplitudes, facilitating their computation.

Abstract

We uncover surprising hidden simplicity in Mellin amplitudes for tree-level AdS holographic correlators for spinning operators, such as AdS "gluons" and "gravitons" (spin 1 and 2). We define Mellin amplitudes with $n$ spinning operators via the so-called "scaffolding" of $2n$-scalar ones with specific projection operators for each spin state, which are rational functions of Mellin variables of $2n$ scalars generalizing flat-space scaffolding amplitudes. We classify possible three-point structures with spin 1 and 2 which take the same form as massive three-point amplitudes in flat space, and match with special solutions such as those extracted from 6-scalar ones in $\mathrm{AdS}_5\times S^3$ or $\mathrm{AdS}_5\times S^5$. Focusing on $\mathrm{AdS}_5$ gluons, we directly bootstrap spinning amplitudes in scaffolding form up to $n=6$ gluons (which amounts to $2n=12$ scalars) using factorizations, multi-linearity and flat-space limit. The results take a remarkably simple form in analogy with flat-space amplitudes, which can be constructed from familiar 3- and 4-vertices as well as propagators of massive spin-1 particles. Surprisingly, we find that vertices with any descendant levels are proportional to the primary ones with nice combinatorial coefficients, which makes manifest the correct flat-space limit in the simplest possible way.