  We examine the phase diagram of the spin-$1$ $J_1-J_2-J_3$ ferromagnetic
Heisenberg model with an easy-plane crystal field on the cubic lattice, in
which $J_1$ is the ferromagnetic exchange interaction between nearest
neighbors, $J_2$ is the antiferromagnetic exchange interaction between
next-nearest neighbors and $J_3$ is the antiferromagnetic exchange interaction
between next-next-nearest neighbors. Using the bond-operator formalism, we
investigate the phase transitions between the disordered paramagnetic phase and
the ordered ones.
  We show that the nature of the quantum phase transitions change as the
frustration parameters ($\frac{J_2}{J_1}$, $\frac{J_3}{J_1}$) are varied. The
zero-temperature phase diagram exhibits second- and first-order transitions,
depending on the energy gap behavior. Remarkably, we find a disordered
nonmagnetic phase, even in the absence of a crystal field, which is suggested
to be a quantum spin liquid candidate. We also depict the phase diagram at
finite temperature for some values of crystal field and frustration parameters.
