A simple version of the Bardeen-Cooper-Schrieffer (BCS)-type mean-field theory for the $t\ensuremath{-}J$ model is developed. The present approach rigorously treats the constraint of no doubly occupied states and invokes two local order parameters to implement spontaneous breaking of the global $\mathrm{U}(1)\ifmmode\times\else\texttimes\fi{}\mathrm{U}(1)$ symmetry. This is achieved by identifying the Hubbard operators with generators of the
SU(2∣1) superalgebra in the fundamental representation and employing the ensuing
CP1∣1 parametrization for dynamical variables. As a result, an improved phase diagram ${T}_{c}(\ensuremath{\delta})$ in the paramagnetic phase is obtained.