In the self-dual higher-spin theory, a scalar vacuum that breaks AdS symmetry to 3D Poincaré makes all higher-spin gauge fields decouple except spin one, and makes higher-spin currents non-conserved except the spin-one current.
Moderately non-local $\eta \bar\eta$ vertices in the $AdS_4$ higher-spin gauge theory
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abstract
A new concept of moderate non-locality in higher-spin gauge theory is introduced. Based on the recently proposed differential homotopy approach, a moderately non-local scheme, that issofter than those resulting from the shifted homotopy approach available in the literature so far, is worked out in the mixed $\eta\bar\eta$ sector of the Vasiliev higher-spin theory. To calculate moderately non-local vertices $\Upsilon^{\eta\bar \eta}(\omega, C,C,C)$ for all ordering of the fields $\omega$ and $C$ we apply an interpolating homotopy, that respects the moderate non-locality in the perturbative analysis of the higher-spin equations.
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On symmetry breaking in the self-dual higher-spin theory
In the self-dual higher-spin theory, a scalar vacuum that breaks AdS symmetry to 3D Poincaré makes all higher-spin gauge fields decouple except spin one, and makes higher-spin currents non-conserved except the spin-one current.