Ab initio study of ground and excited states of NiO(100) monolayer

Ab initio periodic Hartree-Fock calculations are reported of ground and d - -> d excited states of an unsupported NiO(100) monolayer in the ferromagnet ic, ferrimagnetic, antiferromagnetic and fully frustrated spin alignments a s a function of the lattice constant. The ground state is found to be highl y ionic and insulating with a minimum energy lattice constant of 4.0 Angstr om. The Ni(d(8)) configuration is [xz)(2)(xy)(2)(xy)(2)(z(2))(1) (x(2) - y( 2))(1)], as found Previously for the bulk, despite the reduced dimensionali ty leading to a reduction in the number of nearest neighbours and differenc e in the ligand-field ordering. The valence band DOS resembles closely that of the bulk with a majority weight of O(p) states at the upper edge leadin g to a charge-transfer system. The Ni d states occur similar to 1 eV below the O(p) band and are dispersed over similar to 4.5 eV in three distinct su b-bands. The relative stability of the four spin alignments is antiferromag netic > ferrimagnetic > ferromagnetic > fully frustrated, with differences in energy of 10.779 meV, 10.017 meV and 1.675 meV respectively at 4.0 Angst rom. Values of -0.84 meV and -10.78 meV can be deduced for the direct spin- spin, Ed, and superexchange, E-se, interaction energies respectively, which compare with values of -1.5 meV and -7.0 meV found previously for the bulk at a lattice constant of 4.265 Angstrom. E-se is found to decrease rapidly to -3.66 meV at 4.5 Angstrom, unlike E-d which remains fairly constant. Th is reduction in E-se is attributed largely to the increase in the band gap of the monolayer compared with the bulk. For the ferromagnetic spin alignme nt at 4.0 Angstrom variationally converged solutions have been obtained for the one-electron d(xy) --> d(z)2, d(xy) --> d(x2-y2) and spin-forbidden d( x2-y2) --> d(z2) excited states and the two-electron d(xy)/d(yz) --> d(z2)/ d(x2-y2) excited state with excitation energies of 1.16 eV, 1.09 eV, 1.84 e V and 1.79 eV respectively. These are close to values that have been deduce d from optical and EEL spectra and high-level cluster calculations. Converg ed solutions for the d(xy) --> d(z2) excited state in the ferromagnetic ali gnment have been obtained for the concentration range 1-4 excited states pe r x 2 unit cell and in the other spin alignments for complete excitation at lattice constants from 3.9 to 5.0 Angstrom. These show d(xy) --> d(z2) exc itations, and by implication other d --> d excitations, to be highly local with an interaction energy of < 0.1 eV per excitation at saturation, to be independent of the spin alignment and to increase slightly with lattice con stant. The favourable arrangement of the nearest neighbour unpaired spins i n the d(xy) --> d(z2) excited state leads to values of E-d, the direct spin -spin coupling energy, which are an order of magnitude greater than the gro und state values and appreciably in excess of the bulk value. E-se, on the other hand, remains approximately the same. The first ionized state is foun d to be essentially d(8)L, as it is in the bulk, with strong localization o f the hole in a p(pi) orbital of a single O atom and retention of the local Ni moments. ;By direct analogy with the changes in the oxygen k-edge spect rum of LixNi1-xO the band gap in the NiO(100) monolayer is estimated to be similar to 5.3 eV from the gap between the hole band and the conduction ban d edge. The first electron addition state is found to be essentially d(9)[(d(z2))(2 )]. The energy of the single charge-transfer excitonic state of a 2 x 2 uni t cell is estimated to be to be similar to 5.6 eV, in close agreement with the band gap deduced from the DOS of the first ionized state.