TY - JOUR
T1 - Substitution effects in zintl phases
T2 - Synthesis and crystal structure of the novel phases Ae3Sn4-xBi1-x (x ≤ 1; Ae = Sr, Ba) ontaining shubnikov-type nets ∞2[Sn 4-xBix]
AU - Ponou, Siméon
AU - Kim, Sung Jin
AU - Fässler, Thomas F.
PY - 2007
Y1 - 2007
N2 - The compounds Ae3Sn4-xBi1+x (Ae = Sr, Ba) with x < 1 have been synthesized by solid-state reactions in welded Nb tubes at high temperature. Their structures were determined by single crystal X-ray diffraction studies to be tetragonal; space group I4/mcm (No. 140); Z = 4, with a = 8.968(1) Å, c = 12.859(1) Å for Sr3Sn 3.36Bi1.64(3) (1) and a = 9.248(2), c = 13.323(3) Å for Ba3Sn3.16Bi1.84(3) (2). The structure consists of two interpenetrating networks formed by a 3D Ae6/2Bi substructure (anti-ReO3 type) forming the host, and layers of interconnected four-member units [Sn4-xBix] with "butterfly"-like shape as the guest. According to the Zintl-Klemm concept, the compounds are slightly electron deficient and will be charge balanced for x = 1. The electronic structures of Ae3Sn 4-xBi1-x calculated by the TB-LMTO-ASA method indicate that the compounds correspond to ideal semiconducting Zintl phases with a narrow band gap for x = 1 (zero-gap semiconductor). The origin of the slight deviation from the optimal electron count for a valance compound is discussed.
AB - The compounds Ae3Sn4-xBi1+x (Ae = Sr, Ba) with x < 1 have been synthesized by solid-state reactions in welded Nb tubes at high temperature. Their structures were determined by single crystal X-ray diffraction studies to be tetragonal; space group I4/mcm (No. 140); Z = 4, with a = 8.968(1) Å, c = 12.859(1) Å for Sr3Sn 3.36Bi1.64(3) (1) and a = 9.248(2), c = 13.323(3) Å for Ba3Sn3.16Bi1.84(3) (2). The structure consists of two interpenetrating networks formed by a 3D Ae6/2Bi substructure (anti-ReO3 type) forming the host, and layers of interconnected four-member units [Sn4-xBix] with "butterfly"-like shape as the guest. According to the Zintl-Klemm concept, the compounds are slightly electron deficient and will be charge balanced for x = 1. The electronic structures of Ae3Sn 4-xBi1-x calculated by the TB-LMTO-ASA method indicate that the compounds correspond to ideal semiconducting Zintl phases with a narrow band gap for x = 1 (zero-gap semiconductor). The origin of the slight deviation from the optimal electron count for a valance compound is discussed.
KW - Bismuth
KW - Crystal structure
KW - Electronic structure
KW - Intermetallic compound
KW - Tin
KW - Zero-gap semiconductor
UR - http://www.scopus.com/inward/record.url?scp=34548073573&partnerID=8YFLogxK
U2 - 10.1002/zaac.200700213
DO - 10.1002/zaac.200700213
M3 - Article
AN - SCOPUS:34548073573
SN - 0044-2313
VL - 633
SP - 1568
EP - 1574
JO - Zeitschrift fur Anorganische und Allgemeine Chemie
JF - Zeitschrift fur Anorganische und Allgemeine Chemie
IS - 10
ER -