Praseodymium diiodide, PrI2, revisited by synthesis, structure determination and theory

被引:20
作者
Gerlitzki, N
Meyer, G
Mudring, AV
Corbett, JD
机构
[1] Univ Cologne, Inst Anorgan Chem, D-50939 Cologne, Germany
[2] Iowa State Univ Sci & Technol, Ames Lab, Ames, IA 50011 USA
[3] Iowa State Univ Sci & Technol, Dept Chem, Ames, IA 50011 USA
关键词
praseodymium diiodide; crystal structures; band structure;
D O I
10.1016/j.jallcom.2004.03.046
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
Praseodymium diiodide, PrI2, is obtained from the triiodide, PrI3, by reduction with praseodymium metal at elevated temperatures. The two modifications, PrI2-IV and -V, are obtained in different ratios upon fast and slow cooling, respectively. PrI2-IV crystallizes with the CdCl2 type of structure (trigonal, R-3m, a = 426.5(1), c = 2247.1(8) pm) while PrI2-V (cubic, F-43m, a = 1239.9(2) pm) represents an own structure type that may be considered as a structural variant of the CdCl2 type with tetrahedral Pr-4 clusters. To elucidate the electronic properties of the modifications of PrI2 first principles electronic band structure calculations have been carried out using the tight-binding linear-muffin-tin-orbital method (LMTO) as well as the full potential augmented plane wave method (FP-LAPW). The band structure and the bonding were analysed in terms of projections of the bands onto orthogonal orbitals. It was especially focussed on Pr-Pr interactions by crystal orbital Hamiltonian population (COHP) analysis. The calculations show accordingly that a configurational crossover between a [Xe]6s(0)5d(0)4f(n) and a [Xe]6s(0)5d(1)4f(n-1) configuration can be observed in the case of PrI2, depending upon the structure adopted. A higher d orbital contribution results in stronger Pr-Pr interactions. Thus, the driving force appears to be an optimisation of bonding. (C) 2004 Elsevier B.V. All rights reserved.
引用
收藏
页码:211 / 218
页数:8
相关论文
共 36 条
[1]   EXPLICIT, 1ST-PRINCIPLES TIGHT-BINDING THEORY [J].
ANDERSEN, OK ;
JEPSEN, O .
PHYSICAL REVIEW LETTERS, 1984, 53 (27) :2571-2574
[2]  
BECK HP, 1976, Z NATURFORSCH B, V31, P1548
[3]   FULL-POTENTIAL, LINEARIZED AUGMENTED PLANE-WAVE PROGRAMS FOR CRYSTALLINE SYSTEMS [J].
BLAHA, P ;
SCHWARZ, K ;
SORANTIN, P ;
TRICKEY, SB .
COMPUTER PHYSICS COMMUNICATIONS, 1990, 59 (02) :399-415
[4]  
Blaha P., 2001, WIEN2K
[5]  
Blochl P., 1994, PHYS REV B, VB 34, P16223
[6]  
CORBETT JD, 1983, INORG SYN, V22, P36
[7]  
CORBETT JD, 1967, ADV CHEM SER, P56
[8]  
CORBETT JD, 1961, DISCUSS FARADAY SOC, P79
[9]  
CORBETT JD, 1973, REV CHIM MINER, V10, P259
[10]  
Desclaux J., 1969, COMPUT PHYS COMMUN, V1, P216