Cs3LiZn2(WO4)4 and Rb3Li2Ga(MoO4)4: different filled derivatives of the cation-deficient Cs6Zn5(MoO4)8 structure

Two new compounds, namely cubic tricaesium lithium dizinc tetrakis(tetraoxotungstate), Cs3LiZn2(WO4)(4), and tetragonal trirubidium dilithium gallium tetrakis(tetraoxomolybdate), Rb3Li2Ga(MoO4)(4), belong to the structural family of Cs6Zn5(MoO4)(8) (space group I (4) over bar 3d, Z = 4), with a partially incomplete (Zn-5/6 square 1/6) position. In Cs3LiZn2(WO4)(4), this position is fully statistically occupied by (Zn2/3Li1/3), and in Rb3Li2Ga(MoO4)(4), the 2Li(+) Ga atoms are completely ordered in two distinct sites of the space group I(42)d (Z = 4). In the same way, the crystallographically equivalent A + cations (A = Cs, Rb) in Cs6Zn5(MoO4)(8), Cs-3 LiZn2(WO4)(4) and isostructural A(3)LiZn(2)(MoO4)(4) and Cs3LiCo2(MoO4)(4) are divided into two sites in Rb3Li2Ga(MoO4()4), as in other isostructural A(3)Li(2)R(MoO4)(4) compounds (AR = TlAl, RbAl, CsAl, CsGa, CsFe). In the title structures, the WO4 and (Zn, Li)O-4 or LiO4, GaO4 and MoO4 tetrahedra share corners to form open three-dimensional frameworks with the caesium or rubidium ions occupying cuboctahedral cavities. The tetrahedral frameworks are related to that of mayenite 12CaO center dot 7Al(2)O(3) and isotypic compounds. Comparison of isostructural Cs3MZn2(MoO4)(4) (M = Li, Na, Ag) and Cs6Zn5(MoO4)(8) shows a decrease of the cubic lattice parameter and an increase in thermal stability with the filling of the vacancies by Li + in the Zn position of the Cs6Zn5(MoO4)(8) structure, while filling of the cation vacancies by larger Na+ or Ag+ ions plays a destabilizing role. The series A(3)Li(2)R(MoO4)(4) shows second harmonic generation effects compatible with that of beta'-Gd-2(MoO4)(3) and may be considered as nonlinear optical materials with a modest nonlinearity.