The crystal structure of TlAlSiO4:: The role of inert pairs in exclusion of Tl from silicate minerals

被引:13
作者
Kyono, A [1 ]
Kimata, M [1 ]
Shimizu, M [1 ]
机构
[1] Univ Tsukuba, Inst Geosci, Tsukuba, Ibaraki 3058571, Japan
关键词
D O I
10.2138/am-2000-8-921
中图分类号
P3 [地球物理学]; P59 [地球化学];
学科分类号
0708 ; 070902 ;
摘要
Thallium aluminosilicate, TlAlSiO4, synthesized hydrothermally is monoclinic with space group P2(1)/n [a = 5.4095(3), b = 9.4232(7), c = 8.2629(6) Angstrom, gamma = 90.01(2)degrees, V= 421.20(6) Angstrom(3), Z = 4]. Th, crystal structure was refined to an R index of 3.8% based on 1852 observed unique reflections. The compound is a unique framework silicate with a topology similar to that of the tridymite structure. The TlO8 polyhedron resembles a truncated rectangular pyramid, and shares its edges with three adjacent AlO4 tetrahedra, three SiO4 tetrahedra, and six TlO8 polyhedra. Local understaturation at the Tl position suggested by bond-valence analysis implies that lone-pair electrons are present. The geometrical data indicate that the inert pair causes distortion of the Tl-polyhedron. Polyhedral distortion analysis using the software IVTON places the lone-pair parallel to [010], pointing to the largest base of Tl polyhedron. The rule in the valence shell electron pair repulsion model that a nonbonding pair occupies more space on the "surface" of the central atom than a bonding pair supports the orientation of inert-pair electrons in thallium provided by IVTON. The remarkable structure distortion caused by the inert-pair effect explains the rarity of Tl as a major element in silicate minerals because these cannot accommodate extremely distorted polyhedra. In contrast, about forty species of Tl-sulfide minerals exist because these structures are more flexible. Furthermore this effect probably explains why atoms such as Ge2+, Pb2+, Sn2+, Sb3+, and Bi3+, crystallize not as silicate phases but mainly as sulfide ones in nature.
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页码:1287 / 1293
页数:7
相关论文
共 50 条
[1]  
[Anonymous], MOL GEOMETRY
[2]  
[Anonymous], 1993, HEYS MINERAL INDEX M
[3]  
ARAKI T, 1981, AM MINERAL, V66, P1263
[4]   X-RAY STUDY OF LICSSO4 IN CONNECTION WITH ITS FERROELASTIC PHASE-TRANSITION [J].
ASAHI, T ;
HASEBE, K .
JOURNAL OF THE PHYSICAL SOCIETY OF JAPAN, 1988, 57 (12) :4184-4190
[5]   Structure determination of ferromagnetic perovskite BiMnO3 [J].
Atou, T ;
Chiba, H ;
Ohoyama, K ;
Yamaguchi, Y ;
Syono, Y .
JOURNAL OF SOLID STATE CHEMISTRY, 1999, 145 (02) :639-642
[6]   REFINEMENT OF CRYSTAL-STRUCTURE OF STIBNITE, SB2S3 [J].
BAYLISS, P ;
NOWACKI, W .
ZEITSCHRIFT FUR KRISTALLOGRAPHIE KRISTALLGEOMETRIE KRISTALLPHYSIK KRISTALLCHEMIE, 1972, 135 (3-4) :308-&
[7]  
Berlepsch P, 1996, SCHWEIZ MINER PETROG, V76, P147
[8]   BOND-VALENCE PARAMETERS FOR SOLIDS [J].
BRESE, NE ;
OKEEFFE, M .
ACTA CRYSTALLOGRAPHICA SECTION B-STRUCTURAL SCIENCE, 1991, 47 :192-197
[9]   Eightfold superstructure in K2Gd2Sb2Se9 and K2La2Sb2S9 caused by three-dimensional ordering of the 5s2 lone pair of Sb3+ ions [J].
Choi, KS ;
Hanko, JA ;
Kanatzidis, MG .
JOURNAL OF SOLID STATE CHEMISTRY, 1999, 147 (01) :309-319
[10]  
Cooper MA, 1999, CAN MINERAL, V37, P915