We consider scalar field theories invariant under extended shift symmetries
consisting of higher order polynomials in the spacetime coordinates. These
generalize ordinary shift symmetries and the linear shift symmetries of the
galileons. We find Wess-Zumino Lagrangians which transform up to total
derivatives under these symmetries, and which possess fewer derivatives per
field and lower order equations of motion than the strictly invariant terms. In
the non-relativistic context, where the extended shifts are purely spatial,
these theories may describe multi-critical Goldstone bosons. In the
relativistic case, where the shifts involve the full spacetime coordinate,
these theories generally propagate extra ghostly degrees of freedom.Comment: 26 pages. v2: typos, references correcte