  We study invertible states of 1d bosonic quantum lattice systems. We show
that every invertible 1d state is in a trivial phase: after tensoring with some
unentangled ancillas it can be disentangled by a fuzzy analog of a finite-depth
quantum circuit. If an invertible state has symmetries, it may be impossible to
disentangle it in a way that preserves the symmetries, even after adding
unentagled ancillas. We show that in the case of a finite unitary symmetry G
the only obstruction is an index valued in degree-2 cohomology of $G$. We show
that two invertible $G$-invariant states are in the same phase if and only if
their indices coincide.
