Compounds of berkelium
Berkelium forms a number of chemical compounds, where it normally exists in an oxidation state of +3 or +4, and behaves similarly to its lanthanide analogue, terbium. Like all actinides, berkelium easily dissolves in various aqueous inorganic acids, liberating gaseous hydrogen and converting into the trivalent oxidation state. This trivalent state is the most stable, especially in aqueous solutions, but tetravalent berkelium compounds are also known. The existence of divalent berkelium salts is uncertain and has only been reported in mixed lanthanum chloride-strontium chloride melts. Aqueous solutions of Bk3+ ions are green in most acids. The color of the Bk4+ ions is yellow in hydrochloric acid and orange-yellow in sulfuric acid. Berkelium does not react rapidly with oxygen at room temperature, possibly due to the formation of a protective oxide surface layer; however, it reacts with molten metals, hydrogen, halogens, chalcogens and pnictogens to form various binary compounds. Berkelium can also form several organometallic compounds.
Two oxides of berkelium are known, with berkelium in the +3 (Bk2O3) and +4 (BkO2) oxidation states. Berkelium(IV) oxide is a brown solid that crystallizes in a cubic (fluorite) crystal structure with the space group Fm3m and the coordination numbers of Bk and O. The lattice parameter is 533.4 ± 0.5 pm.
The compound has a melting point of 1920 °C, body-centered cubic crystal lattice and a lattice constant a = 1088.0 ± 0.5 pm. Upon heating to 1200 °C, the cubic Bk2O3 transforms to a monoclinic structure, which further converts to a hexagonal phase at 1750 °C; the latter transition is reversible. Such three-phase behavior is typical for the actinide sesquioxides.
In halides, berkelium assumes the oxidation states +3 and +4. The +3 state is most stable, especially in solutions, and the tetravalent halides BkF4 and Cs2BkCl6 are only known in the solid phase. The coordination of the berkelium atom in its trivalent fluoride and chloride is tricapped trigonal prismatic, with a coordination number of 9. In the trivalent bromide, it is bicapped trigonal prismatic (coordination 8) or octahedral (coordination 6), and in the iodide it is octahedral.
Berkelium(IV) fluoride (BkF4) is a yellow-green ionic solid which crystallizes in the monoclinic crystal system (Pearson symbol mS60, space group C2/c No. 15, lattice constants a = 1247 pm, b = 1058 pm, c = 817 pm) and is isotypic with uranium tetrafluoride or zirconium(IV) fluoride.
Berkelium(III) fluoride (BkF3) is also a yellow-green solid, but it has two crystalline structures. The most stable phase at low temperatures has an orthorhombic symmetry, isotypic with yttrium(III) fluoride (Pearson symbol oP16, space group Pnma, No. 62, a = 670 pm, b = 709 pm, c = 441 pm). Upon heating to 350 to 600 °C, it transforms to a trigonal structure found in lanthanum(III) fluoride (Pearson symbol hP24, space group P3c1, No. 165, a = 697 pm, c = 714 pm).
Visible amounts of berkelium(III) chloride (BkCl3) were first isolated and characterized in 1962, and weighed only 3 billionths of a gram. It can be prepared by introducing hydrogen chloride vapors into an evacuated quartz tube containing berkelium oxide at a temperature of about 500 °C. This green solid has a melting point of 603 °C and crystallizes in the hexagonal crystal system isotypic with uranium(III) chloride (Pearson symbol hP8, space group P63/m, No. 176). Upon heating to just below its melting point, BkCl3 converts into an orthorhombic phase. The hexahydrate BkCl3·6H2O (berkelium trichloride hexahydrate) has a monoclinic structure with the lattice constants a = 966 pm, b = 654 pm and c = 797 pm. Another berkelium(III) chloride, Cs2NaBkCl6 can be crystallized from a chilled aqueous solution containing berkelium(III) hydroxide, hydrochloric acid and caesium chloride. It has a face-centered cubic structure where Bk(III) ions are surrounded by chloride ions in an octahedral configuration.
The ternary berkelium(IV) chloride Cs2BkCl6 is obtained by dissolving berkelium(IV) hydroxide in a chilled solution of caesium chloride in concentrated hydrochloric acid. It forms orange hexagonal crystals with the lattice constants a = 745.1 pm and c = 1209.7 pm. The average radius of the BkCl62– ion in this compound is estimated as 270 pm.
Two forms of berkelium(III) bromide are known, a monoclinic with berkelium coordination 6 and orthorhombic with coordination 8; the latter is less stable and transforms to the former phase upon heating to about 350 °C. An important phenomenon for radioactive solids has been studied for these two crystal forms: the structures of fresh and aged 249BkBr3 samples were studied using X-ray diffraction over a period longer than 3 years, so that various fractions of 249Bk had beta decayed to 249Cf. No change in structure was observed upon the 249BkBr3—249CfBr3 transformation, even though the orthorhombic bromide was previously unknown for californium. However, other differences were noted for 249BkBr3 and 249CfBr3. For example, the latter could be reduced with hydrogen to249CfBr2, but the former could be not – this result was reproduced on individual 249BkBr3 and249CfBr3 samples, as well on the samples containing both bromides. The intergrowth of californium in berkelium occurs at a rate of 0.22% per day and is an intrinsic obstacle in studying berkelium properties. Besides a chemical contamination, 249Cf, as an alpha emitter brings undesirable self-damage of the crystal lattice due to the resulting self-heating. This can be avoided by performing measurements as a function of time and extrapolating the obtained results.
Berkelium(III) iodide forms hexagonal crystals with the lattice constants a = 758.4 pm and c = 2087 pm. The known oxyhalides of berkelium include BkOCl, BkOBr and BkOI; they all crystallize in a tetragonal lattice.
Other inorganic compounds
The monopnictides of berkelium-249 are known for the elements nitrogen, phosphorus, arsenic and antimony. They are prepared by the reaction of either berkelium(III) hydride (BkH3) or metallic berkelium with these elements at elevated temperatures (about 600 °C) under high vacuum in quartz ampoules. They crystallize in the cubic crystal system with the lattice constant of 495.1 pm for BkN, 566.9 pm for BkP, 582.9 for BkAs and 619.1 pm for BkSb. These lattice constant values are smaller than those in curium pnictides, but are comparable to those of terbium pnictides.
Berkelium(III) sulfide, Bk2S3, has been prepared by either treating berkelium oxide with a mixture of hydrogen sulfide and carbon disulfidevapors at 1130 °C, or by directly reacting metallic berkelium with sulfur. These procedures yield brownish-black crystals with a cubic symmetry and lattice constant a = 844 pm.
Berkelium(III) and berkelium(IV) hydroxides are both stable in 1 M sodium hydroxide solutions. Berkelium(III) phosphate (BkPO4) has been prepared as a solid, which shows strong fluorescence under argon laser (514.5 nm line) excitation. Berkelium hydrides are produced by reacting metal with hydrogen gas at temperatures about 250 °C. They are non-stoichiometric with the nominal formula BkH2+x (0 < x < 1). Whereas the trihydride has a hexagonal symmetry, the dihydride crystallizes in an fcc structure with the lattice constant a = 523 pm. Several other salts of berkelium are known, including Bk2O2S, (BkNO3)3·4H2O, BkCl3·6H2O, Bk2(SO4)3·12H2O and Bk2(C2O4)3·4H2O. Thermal decomposition at about 600 °C in an argon atmosphere (to avoid oxidation to Bk2O) of Bk2(SO4)3·12H2O yields the body-centered orthorhombic crystals of berkelium(IV) oxysulfate (Bk2O2SO4). This compound is thermally stable to at least 1000 °C in an inert atmosphere.
Berkelium forms a trigonal (η5–C5H5)3Bk complex with three cyclopentadienyl rings, which can be synthesized by reacting berkelium(III) chloride with the molten beryllocene Be(C5H5)2 at about 70 °C. It has an amber color and orthorhombic symmetry, with the lattice constants of a = 1411 pm, b = 1755 pm and c = 963 pm and the calculated density of 2.47 g/cm3. The complex is stable to heating to at least 250 °C, and sublimates without melting at about 350 °C. The high radioactivity of berkelium gradually destroys the compound within a period of weeks. One C5H5 ring in (η5–C5H5)3Bk can be substituted by chlorine to yield [Bk(C5H5)2Cl]2. The optical absorption spectra of this compound are very similar to those of (η5–C5H5)3Bk.
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- Greenwood, Norman N.; Earnshaw, Alan (1997). Chemistry of the Elements (2nd ed.). Butterworth-Heinemann. ISBN 0080379419.
- Holleman, Arnold F. and Wiberg, Nils Textbook of Inorganic Chemistry, 102 Edition, de Gruyter, Berlin 2007, ISBN 978-3-11-017770-1.
- Peterson J. R. and Hobart D. E. "The Chemistry of Berkelium" in Harry Julius Emeléus (Ed.) Advances in inorganic chemistry and radiochemistry, Volume 28, Academic Press, 1984 ISBN 0-12-023628-1, pp. 29–64, doi:10.1016/S0898-8838(08)60204-4