Shifted Homotopy Analysis of the Linearized Higher-Spin Equations in Arbitrary Higher-Spin Background

TL;DR

This paper extends the analysis of higher-spin equations by introducing shifted homotopy operators, revealing a new class of vertices that preserve the equations' proper form and showing that certain shifts do not affect the first-order fields.

Contribution

It introduces shifted homotopy operators in higher-spin equations, expanding the class of vertices while maintaining the equations' proper form and invariance properties.

Findings

Relaxed uniform (y+p)-shift respects the proper form of free higher-spin equations.

Shift by the argument of (Y) does not affect the first-order higher-spin field W.

The new class of vertices includes those from conventional no-shift homotopy.

Abstract

Analysis of the first-order corrections to higher-spin equations is extended to homotopy operators involving shift parameters with respect to the spinor $Y$ variables, the argument of the higher-spin connection $\omega(Y)$ and the argument of the higher-spin zero-form $C(Y)$. It is shown that a relaxed uniform $(y+p)$-shift and a shift by the argument of $\omega(Y)$ respect the proper form of the free higher-spin equations and constitute a one-parametric class of vertices that contains those resulting from the conventional (no shift) homotopy. A pure shift by the argument of $\omega(Y)$ is shown not to affect the one-form higher-spin field $W$ in the first order and, hence, the form of the respective vertices.