The anomalous magnetic phase transition in UNiSn is explained on the b
asis of electronic-structure calculations. The energy band approach in
which the local density Hamiltonian is generalized with an additional
on-site Coulomb interaction U provides a fully satisfactory picture o
f both the metallic antiferromagnetic ground state and the paramagneti
c semiconducting state, with a band gap of 0.12 eV, as well as a total
energy difference of the correct magnitude as compared to the Neel te
mperature.