The 5f (2)- 5f (1)6d(1) absorption spectrum of Cs2GeF6 : U4+ crystals: A quantum chemical and experimental study

摘要

Single crystals of U4+-doped Cs2GeF6 with 1% U4+ concentration have been obtained by the modified Bridgman-Stockbarger method in spite of the large difference in ionic radii between Ge4+ and U4+ in octahedral coordination. Their UV absorption spectrum has been recorded at 7 K, between 190 and 350 nm; it consists of a first broad and intense band peaking at about 38 000 cm(-1) followed by a number of broad bands of lower intensity from 39 000 to 45 000 cm(-1). None of the bands observed shows appreciable fine vibronic structure, so that the energies of experimental electronic origins cannot be deduced and the assignment of the experimental spectrum using empirical methods based on crystal field theory cannot be attempted. Alternatively, the profile of the absorption spectrum has been obtained theoretically using the U-F bond lengths and totally symmetric vibrational frequencies of the ground 5f(2)-1A(1g) and 5f(1)6d(t(2g))(1)-iT(1u) excited states, their energy differences, and their corresponding electric dipole transition moments calculated using the relativistic ab initio model potential embedded cluster method. The calculations suggest that the observed bands are associated with the lowest five 5f(2)-1A(1g)-> 5f(1)6d(t(2g))(1)-iT(1u) (i=1-5) dipole allowed electronic origins and their vibrational progressions. In particular, the first broad and intense band peaking at about 38 000 cm(-1) can be safely assigned to the 0-0 and 0-1 members of the a(1g) progression of the 5f(2)-1A(1g)-> 5f(1)6d(t(2g))(1)-1T(1u) electronic origin. The electronic structure of all the states with main configurational character 5f(1)6d(t(2g))(1) has been calculated as well. The results show that the lowest crystal level of this manifold is 5f(1)6d(t(2g))(1)-1E(u) and lies about 6200 cm(-1) above the 5f(2) level closest in energy, which amounts to some 11 vibrational quanta. This large energy gap could result in low nonradiative decay and efficient UV emission, which suggest the interest of investigating further this new material as a potential UV solid state laser. (c) 2006 American Institute of Physics.