Abstract
The spin-density functional formalism is investigated with the objective of producing practical methods for calculating the spin (magnetic moment) density, m(r), of atoms, molecules, and metals. Calculations are performed for the atoms Li, Na, K, N, P, Mn, and As in their spherically symmetric ground states using two approximations for the exchange-correlation functional: (i) the exact treatment of exchange with a local approximation for correlation (referred to as "SUHF-C"), (ii) the local spin-density (LSD) approximation for both exchange and correlation. The "SUHF-C" values of m(0) for Li, Na, K, N, P, Mn, and As are 108, 99, 91, 200, -30, 108, and 93% of experiment, respectively. For Li, Na, and K the LSD approximation yields 98, 109, and 106%, respectively. Away from the nucleus, in all the cases studied, the LSD and "SUHF-C" results for m(r) are in close agreement. We conclude that for systems where there is a large direct contribution the LSD approximation should give better than 90% accuracy, even at the origin. The results using "SUHF-C" suggest that it has the capability of yielding accurate values of m(r) for atoms and molecules.