The participation of the valence orbitals of actinides in bonding has been debated for decades. Recent experimental and computational investigations demonstrated the involvement of 6p, 6d and/or 5f orbitals in bonding. However, structural and spectroscopic data, as well as theory, indicate a decrease in covalency across the actinide series, and the evidence points to highly ionic, lanthanide-like bonding for late actinides. Here we show that chemical differentiation between californium and lanthanides can be achieved by using ligands that are both highly polarizable and substantially rearrange on complexation. A ligand that suits both of these desired properties is polyborate. We demonstrate that the 5f, 6d and 7p orbitals are all involved in bonding in a Cf(III) borate, and that large crystal-field effects are present. Synthetic, structural and spectroscopic data are complemented by quantum mechanical calculations to support these observations.

A break in periodicity occurs in the actinide series between plutonium and americium as the result of the localization of 5f electrons. The subsequent chemistry of later actinides is thought to closely parallel lanthanides in that bonding is expected to be ionic and complexation should not substantially alter the electronic structure of the metal ions. Here we demonstrate that ligation of californium(III) by a pyridine derivative results in significant deviations in the properties of the resultant complex with respect to that predicted for the free ion. We expand on this by characterizing the americium and curium analogues for comparison, and show that these pronounced effects result from a second transition in periodicity in the actinide series that occurs, in part, because of the stabilization of the divalent oxidation state. The metastability of californium(II) is responsible for many of the unusual properties of californium including the green photoluminescence.

Four uranyl borates, UO(2)B(2)O(4) (UBO-1), alpha-(UO(2))(2)[B(9)O(14)(OH)(4)] (UBO-2), beta-(UO(2))(2)[B(9)O(14)(OH)(4)] (UBO-3), and (UO(2))(2)[B(13)O(20)(OH)(3)].1.25H(2)O (UBO-4), have been prepared from boric acid fluxes at 190 degrees C. UBO-3 and UBO-4 are centrosymmetric, whereas UBO-1 and UBO-2 are noncentrosymmetric (chiral and polar). These uranyl borates possess layered structures constructed from UO(8) hexagonal bipyramids, BO(3) triangles, and BO(4) tetrahedra. In the case of UBO-4, clusters of BO(3) triangles link the layers together to form open slabs with a thickness of almost 2 nm. The ability of uranyl borates to use very similar layers to yield both centrosymmetric and noncentrosymmetric layers is detailed in this work.

The reaction of uranyl nitrate with a large excess of molten boric acid in the presence of potassium or rubidium nitrate results in the formation of three new potassium uranyl borates, K(2)[(UO(2))(2)B(12)O(19)(OH)(4)].0.3H(2)O (KUBO-1), K[(UO(2))(2)B(10)O(15)(OH)(5)] (KUBO-2), and K[(UO(2))(2)B(10)O(16)(OH)(3)].0.7H(2)O (KUBO-3) and two new rubidium uranyl borates Rb(2)[(UO(2))(2)B(13)O(20)(OH)(5)] (RbUBO-1) and Rb[(UO(2))(2)B(10)O(16)(OH)(3)].0.7H(2)O (RbUBO-2). The latter is isotypic with KUBO-3. These compounds share a common structural motif consisting of a linear uranyl, UO(2)(2+), cation surrounded by BO(3) triangles and BO(4) tetrahedra to create an UO(8) hexagonal bipyramidal environment around uranium. The borate anions bridge between uranyl units to create sheets. Additional BO(3) triangles extend from the polyborate layers and are directed approximately perpendicular to the sheets. All of these compounds adopt layered structures. With the exception of KUBO-1, the structures are all centrosymmetric. All of these compounds fluoresce when irradiated with long-wavelength UV light. The fluorescence spectrum yields well-defined vibronically coupled charge-transfer features.

Four new uranyl borates, Li[UO2B5O9]·H2O (LiUBO-1), Ag[(UO2)B5O8(OH)2] (AgUBO-1), α-Cs[(UO2)2B11O16(OH)6] (CsUBO-1), and β-Cs[(UO2)2B11O16(OH)6] (CsUBO-2) were synthesized via the reaction of uranyl nitrate with a large excess of molten boric acid in the presence of lithium, silver, or cesium nitrate. These compounds share a common structural motif consisting of a linear uranyl, UO2 2+, cation surrounded by BO3 triangles and BO4 tetrahedra to create an UO8 hexagonal bipyramidal environment around uranium. The borate anions bridge between uranyl units to create sheets. Additional BO3 triangles extend from the polyborate layers, and are directed approximately perpendicular to the sheets. In Li[(UO2)B5O9]·H2O, the additional BO3 triangles connect these sheets together to form a three-dimensional framework structure. Li[UO2)B5O9]·H2O and β-Cs[(UO2)2B11O16(OH)6] adopt noncentrosymmetric structures, while Ag[(UO2)B5O8(OH)2] and α-Cs[(UO2)2B11O16(OH)6] are centrosymmetric. Li[(UO2)B5O9]·H2O, which can be obtained as pure phase, displays second-harmonic generation of 532 nm light from 1064 nm light. Topological relationships of all actinyl borates are developed.