The phase stability of two-dimensional monolayer As 1−x P x solid solutions, exhibiting the puckered (α phase) and buckled (β phase) structures are investigated using a first-principles cluster-expansion method. Canonical Monte Carlo simulations, together with harmonic approximation, are performed to capture the influences of thermally induced configurational disorder and lattice vibrations on the phase stability of monolayer As 1−x P x. We first demonstrate that, as the temperature approaches 0 K, the monolayer As 1−x P x displays a tendency toward phase separation into its constituent elemental phases, and thus no stable ordered structures of As 1−x P x , both α and β phases, are predicted to be thermodynamically stable. We further reveal with the inclusion of the lattice vibrational contributions that β-As 1−x P x is thermodynamically favored over α-As 1−x P x across the entire composition range even at 0 K and increasingly so at higher temperature, and a continuous series of disordered solid solution of β-As 1−x P x , where 0 x 1, is predicted at the temperature above 550 K. These findings not only indicate that the ordered structures of monolayer α-As 1−x P x and β-As 1−x P x , frequently studied in the literature, may not exist in nature, but also presumably suggest that monolayer α-As 1−x P x is metastable with respect to monolayer β-As 1−x P x .