4.6 Article

Influence of the metal-metal sigma bonding on the structures and physical properties of the hexagonal perovskite-type sulfides Sr9/8TiS3,Sr8/7TiS3, and Sr8/7[Ti6/7Fe1/7]S3

Journal

JOURNAL OF SOLID STATE CHEMISTRY
Volume 162, Issue 1, Pages 103-112

Publisher

ACADEMIC PRESS INC
DOI: 10.1006/jssc.2001.9361

Keywords

-

Ask authors/readers for more resources

The structural and electronic consequences of the metal-metal sigma bonding in the hexagonal perovskite sulfides were examined by calculating the electronic band structures of Sr9/8TiS3 and Sr8/7TiS3, by synthesizing Sr-8/7[Ti6/7Fe1/7]S-3 and characterizing its crystal structure, and by measuring the magnetic susceptibilities of Sr9/8TiS3, Sr8/7TiS3 an Sr-8/7[Ti6/7Fe1/7]S-3. The (TiS3)(infinity) chains of Sr9/8TiS3 and Sr8/7TiS3 contain oligomer units (Oh)(n) (n = 4, 5) made up of face-sharing TiS6 octahedra (Oh)(n) Given the (TiS3)(infinity) chains aligned along the z direction, the only occupied d-block levels of each (TiS3)(infinity) chain are the most sigma bonding level of each (Oh), oligomer, which is constructed from its n z(2) orbitals. This n-orbital two-electron metal-metal sigma bonding controls the d-orbital density distribution and the Ti-Ti distances of the (Oh)(n) oligomers and is ultimately responsible for the semiconducting property of Sr9/8TiS3, Sr8/7TiS3, and Sr-8/7[T6/7Fe1/7]S-3. The Sr-8/7[Ti-6/7 Fe-1/7]S-3 structure is described by the trigonal symmetry, Kim (00y)0s superspace group with the following parameters: a(s) = 11.4935(11) Angstrom, c(s) = 2.9986(7) Angstrom, q = 0.57161(15) c*, and V-s = 343.05(15) Angstrom (3). (C) 2001 Academic Press.

Authors

I am an author on this paper
Click your name to claim this paper and add it to your profile.

Reviews

Primary Rating

4.6
Not enough ratings

Secondary Ratings

Novelty
-
Significance
-
Scientific rigor
-
Rate this paper

Recommended

No Data Available
No Data Available