In this work we study gapped boundary states of bosonic symmetry-protected topological (SPT) phases in 4+1d, which are characterized by mixed -gravity response, and the closely related phases protected by rotation symmetry. We show that if , any symmetry-preserving boundary theory is necessarily gapless for the root SPT state. We then propose a (3+1) gauge theory coupled to fermionic matter as a candidate boundary theory for , where the anomalous symmetry is implemented by invertible topological defects obtained from gauging (2+1) chiral topological superconductors. For the case, we present an explicit construction for the boundary states for , and argue that the construction fails for other values of .

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