  We use the intrinsic one-form and two-form global symmetries of (3+1)$d$
bosonic field theories to classify quantum phases enriched by ordinary
($0$-form) global symmetry. Different symmetry-enriched phases correspond to
different ways of coupling the theory to the background gauge field of the
ordinary symmetry. The input of the classification is the higher-form
symmetries and a permutation action of the $0$-form symmetry on the lines and
surfaces of the theory. From these data we classify the couplings to the
background gauge field by the 0-form symmetry defects constructed from the
higher-form symmetry defects. For trivial two-form symmetry the classification
coincides with the classification for symmetry fractionalizations in $(2+1)d$.
We also provide a systematic method to obtain the symmetry protected
topological phases that can be absorbed by the coupling, and we give the
relative 't Hooft anomaly for different couplings. We discuss several examples
including the gapless pure $U(1)$ gauge theory and the gapped Abelian finite
group gauge theory. As an application, we discover a tension with a conjectured
duality in $(3+1)d$ for $SU(2)$ gauge theory with two adjoint Weyl fermions.
