Complete active-space self-consistent field (CASSCF) method followed by multireference singles + doubles configuration interaction (MRSDCI) calculations that included up to 4 million configurations were carried out on the electronic states of Al 3 P 2 , Al 2 P 3 and their anions and cations. Our computed results explain the recently reported anion photoelectron spectra of Al 2 P 3and Al 3 P 2by Neumark and co-workers. 1 We find that both the Al 2 P 3and Al 2 P 3 species have D 3h undistorted trigonal bipyramidal structures consistent with the sharp and intense ground-state peak in the observed spectra. But the neutral Al 3 P 2 cluster was found to be Jahn-Teller distorted in contrast to the Al 3 P 2anion, which has a D 3h undistorted trigonal bipyramidal structure, consistent with the observed extended vibrational progression of the X state of the spectra. Our computed electron affinities agree well with the onsets of the observed X peaks in both spectra. We assign the partially resolved vibrational structure in the observed spectra to the totally symmetric stretch mode than to symmetry lowering of Al 2 P 3 , which is found to be in a 2 A 2 ′′ (D 3h ) state and cannot undergo Jahn-Teller distortion. Seven electronic states of Al 3 P 2 are computed, among which the 2 A 1 (C 2V ) state is the ground state with a distorted trigonal bipyramid structure. The distorted 2 A 1 and 2 B 1 (C 2V ) states are identified as Jahn-Teller components of the undistorted 2 E′ and 2 E′′ (D 3h ) states, respectively. Properties of four electronic states of Al 2 P 3 , Al 3 P 2 + , and Al 2 P 3 + are also reported. The ground states of both Al 3 P 2 + and Al 2 P 3 + are undistorted 3 A 2 ′ and 1 A 1 ′, respectively (D 3h symmetry). The atomization energy, adiabatic ionization potentials, dipole moments, and other properties for the electronic states of Al 3 P 2 and Al 2 P 3 are calculated and discussed. Comparisons are made with the Ga and In analogues of these species.