Effects of the first hydration sphere and the bulk solvent on the spectra of the f2 isoelectronic actinide compounds: U4+, NpO2+, and PuO22+

被引:29
作者
Danilo, Cecile [1 ,2 ]
Vallet, Valerie [1 ]
Flament, Jean-Pierre [1 ]
Wahlgren, Ulf [2 ,3 ]
机构
[1] Univ Lille 1 Sci & Technol, Lab PhLAM, CNRS, CERLA,UMR 8523,FR 2416, F-59655 Villeneuve Dascq, France
[2] Stockholm Univ, Dept Phys, AlbaNova Univ Ctr, S-10691 Stockholm, Sweden
[3] NORDITA, AlbaNova Univ Ctr, S-10691 Stockholm, Sweden
基金
瑞典研究理事会;
关键词
2ND-ORDER PERTURBATION-THEORY; DENSITY-FUNCTIONAL THEORY; GAUSSIAN-BASIS SETS; ELECTRONIC-STRUCTURE; TETRAVALENT URANIUM; EXCITED-STATES; WATER EXCHANGE; FINE-STRUCTURE; SPIN-ORBIT; AQUA IONS;
D O I
10.1039/b914222c
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
The electronic spectra of the 5f(2) isoelectronic actinide compounds U4+, NpO2+, and PuO22+ have been investigated theoretically both in gas phase and in solution. In the latter case the solvent was modelled by a saturated first hydration sphere, five water molecules for NpO2+, and PuO22+ and eight for U4+, and a continuum model describing the remaining solvent. The transition energies and oscillator strengths were obtained at the spin-orbit level using the relativistic wave function based multi-configuration methods CASPT2 (complete active space with second-order perturbation theory) and MRCI + DC (Davidson corrected multi-reference configuration interaction), followed by a spin-orbit CI based on a dressed effective spin-orbit Hamiltonian. This study is an attempt to contribute to an enhanced understanding of the electronic structure of tetravalent actinide ions and actinyl(V) and (VI) ions. The spin-orbit MRCI and spin-orbit CASPT2 transitions energies have been compared for the bare ions, leading us to the conclusion that the spin-orbit CASPT2 approach is reasonably accurate and can be used with confidence for the calculation of the hydrated species. The first hydration sphere and the bulk solvent lift degeneracies, but the effect on the transition energies is fairly small for the two actinyl ions, while it is larger, up to several thousands of wave numbers for U4+. The calculations allowed us to make assignments of the experimentally observed absorption spectra for all species. The computed transition energies and intensities compared favourably with experiment.
引用
收藏
页码:1116 / 1130
页数:15
相关论文
共 80 条
[1]   Investigation of aquo and chloro complexes of UO22+, NpO2+, Np4+, and Pu3+ by X-ray absorption fine structure spectroscopy [J].
Allen, PG ;
Bucher, JJ ;
Shuh, DK ;
Edelstein, NM ;
Reich, T .
INORGANIC CHEMISTRY, 1997, 36 (21) :4676-4683
[2]   2ND-ORDER PERTURBATION-THEORY WITH A COMPLETE ACTIVE SPACE SELF-CONSISTENT FIELD REFERENCE FUNCTION [J].
ANDERSSON, K ;
MALMQVIST, PA ;
ROOS, BO .
JOURNAL OF CHEMICAL PHYSICS, 1992, 96 (02) :1218-1226
[3]   2ND-ORDER PERTURBATION-THEORY WITH A CASSCF REFERENCE FUNCTION [J].
ANDERSSON, K ;
MALMQVIST, PA ;
ROOS, BO ;
SADLEJ, AJ ;
WOLINSKI, K .
JOURNAL OF PHYSICAL CHEMISTRY, 1990, 94 (14) :5483-5488
[4]   Relativistic XANES calculations of Pu hydrates [J].
Ankudinov, AL ;
Conradson, SD ;
de Leon, JM ;
Rehr, JJ .
PHYSICAL REVIEW B, 1998, 57 (13) :7518-7525
[5]  
Antonio MR, 2001, RADIOCHIM ACTA, V89, P17
[6]   ABSOLUTE OSCILLATOR-STRENGTHS OF 5F-5F TRANSITIONS OF U4+ IN THBR4 AND IN HYDROBROMIC ACID-SOLUTIONS [J].
AUZEL, F ;
HUBERT, S ;
DELAMOYE, P .
JOURNAL OF LUMINESCENCE, 1982, 26 (03) :251-262
[7]   Structure and spectroscopy of U4+ defects in Cs2ZrCl6:: Ab initio theoretical studies on the 5f 2 and 5f 16d1 manifolds [J].
Barandiarán, Z ;
Seijo, L .
JOURNAL OF CHEMICAL PHYSICS, 2003, 118 (16) :7439-7456
[8]  
Bardin N, 1998, RADIOCHIM ACTA, V83, P189
[9]   A new definition of cavities for the computation of solvation free energies by the polarizable continuum model [J].
Barone, V ;
Cossi, M ;
Tomasi, J .
JOURNAL OF CHEMICAL PHYSICS, 1997, 107 (08) :3210-3221
[10]   RAMAN-SCATTERING OF URANYL AND TRANSURANIUM V, VI, AND VII IONS [J].
BASILE, LJ ;
SULLIVAN, JC ;
FERRARO, JR ;
LABONVILLE, P .
APPLIED SPECTROSCOPY, 1974, 28 (02) :142-145