TY - JOUR
T1 - Application of atomic pair distribution function analysis to materials with intrinsic disorder. Three-dimensional structure of exfoliated-restacked WS2
T2 - Not just a random turbostratic assembly of layers
AU - Petkov, V.
AU - Billinge, S. J.L.
AU - Heising, J.
AU - Kanatzidis, M. G.
PY - 2000/11/29
Y1 - 2000/11/29
N2 - The three-dimensional structure of metastable exfoliated-restacked WS2 (r-WS2) has been determined by the atomic pair distribution function (PDF) technique. We show that the structure of r-WS2 is not a random turbostratic assembly of layers, as previously thought, but it can be better regarded as a monoclinic structure with considerable intrinsic disorder. At room temperature, the atomic-scale structure of r-WS2 is well described in the space group P1121 of the monoclinic system with four formula units in the cell, and lattice parameters a = 3.270(5) A, b = 5.717(5) A, c = 12.309(5) A, and γ = 88.43°. Analysis of the X-ray scattering data, collected with Synchrotron radiation (λ = 0.202°) over a wide scattering angle, shows that the metastable material is built of layers of distorted (WS6) octahedral units, in contrast to hexagonal 2H-WS2 which is built of layers of perfect (WS6) trigonal prisms. A characteristic structural feature of the restacked material is that W atoms within a single layer form zigzag chains along the a axis of the unit cell via short metal-metal bonds of length 2.77(1) and 2.85(1) A, in agreement with previous two-dimensional electron diffraction studies.
AB - The three-dimensional structure of metastable exfoliated-restacked WS2 (r-WS2) has been determined by the atomic pair distribution function (PDF) technique. We show that the structure of r-WS2 is not a random turbostratic assembly of layers, as previously thought, but it can be better regarded as a monoclinic structure with considerable intrinsic disorder. At room temperature, the atomic-scale structure of r-WS2 is well described in the space group P1121 of the monoclinic system with four formula units in the cell, and lattice parameters a = 3.270(5) A, b = 5.717(5) A, c = 12.309(5) A, and γ = 88.43°. Analysis of the X-ray scattering data, collected with Synchrotron radiation (λ = 0.202°) over a wide scattering angle, shows that the metastable material is built of layers of distorted (WS6) octahedral units, in contrast to hexagonal 2H-WS2 which is built of layers of perfect (WS6) trigonal prisms. A characteristic structural feature of the restacked material is that W atoms within a single layer form zigzag chains along the a axis of the unit cell via short metal-metal bonds of length 2.77(1) and 2.85(1) A, in agreement with previous two-dimensional electron diffraction studies.
UR - http://www.scopus.com/inward/record.url?scp=0034731018&partnerID=8YFLogxK
U2 - 10.1021/ja002048i
DO - 10.1021/ja002048i
M3 - Article
AN - SCOPUS:0034731018
SN - 0002-7863
VL - 122
SP - 11571
EP - 11576
JO - Journal of the American Chemical Society
JF - Journal of the American Chemical Society
IS - 47
ER -