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Title: Bi{sub {approx}}{sub 3.785}Cd{sub {approx}}{sub 3.575}Cu{sub {approx}}{sub 1.5}(PO{sub 4}){sub 3.5}O{sub 5}= {sub .5}, a new arrangement of double (n=2) and triple (n=3) [M{sub 4}Bi{sub 2n-2}O{sub 2n}]{sup x+} polycationic ribbons in the bismuth-transition metal oxy-phosphate series

Journal Article · · Journal of Solid State Chemistry
 [1];  [1];  [1];  [1]
  1. Laboratoire de Cristallochimie et Physicochimie du Solide, CNRS UMR 8012, ENSCL, Universite des Sciences et Technologies de Lille, BP.108, F-59652 Villeneuve d'Ascq Cedex (France)

This work is dedicated to investigation of new disordered bismuth-containing oxy-phosphates compounds with an original structure type. As previously observed in this series, they are formed of [M{sub 4}Bi{sub 2n-2}O{sub 2n}]{sup x+} polycationic ribbons of width n O(Bi,M){sub 4} tetrahedra, surrounded by PO{sub 4} groups. In the new crystal structure type, double (=D), triple (=T) and tunnels (=t) alternate along a common axis obeying the TtDtTtDt/TTtTTt sequence in respect to a nomenclature previously described and recalled in this work. The existence this new polymorph has first been detected by electron diffraction in a multi-phased sample. Then, the crystal structure type, i.e., the TtDtTtDt/TTtTTt sequence, has been deduced from HREM images help to a contrast-interpreting code available for these series of polycations-formed compounds. The subsequent compounds formulation leads to a number of new materials that verify the general formula: [Bi{sub 2}(Bi,M){sub 4}O{sub 4}]{sub 2} [Bi{sub 4}(Bi,M){sub 4}O{sub 6}]{sub 6} (PO{sub 4}){sub 28} M{sub x}, with x=<12 and M=Cu{sup 2+}, Cd{sup 2+} cations. Single crystals of the nominal [O6Bi{sub 4.57}Cd{sub 3.43}]{sub 4}{sup +8.57} [O{sub 6}Bi{sub 4}Cd{sub 4}]{sub 2}{sup +8} [O{sub 4}Bi{sub 2}Cd{sub 3.56}Cu{sub 0.44}]{sub 2}{sup +6} (PO{sub 4}){sub 28} Cu{sub 10.86} have been prepared in a further stage and confirms the predicted crystal structure, Bi{sub {approx}}{sub 3.785}Cd{sub {approx}}{sub 3.575}Cu{sub {approx}}{sub 1.5}(PO{sub 4}){sub 3.5}O{sub 5.5}= , a=11.506(8)A, b=5.416(4)A, c=53.94 (4)A, {beta}=90.10(1){sup o}, RF=0.0835, RwF=0.0993, SG=A2/m, Z=8. As already observed for other elements of this family such as Bi{sub {approx}}{sub 1.2}M{sub {approx}}{sub 1.2}O{sub 1.5}(PO{sub 4}), Bi{sub {approx}}{sub 6.2}Cu{sub {approx}}{sub 6.2}O{sub 8}(PO{sub 4}){sub 5} or Bi{sub {approx}}{sub 3}Cd{sub {approx}}{sub 3.72}M{sub {approx}}{sub 1.28}O{sub 5}(PO{sub 4}){sub 3} (M=Cu, Co, Zn), this compound shows an additional example of PO{sub 4} disorder due to the presence of mixed Bi{sup 3+}/M{sup 2+} sites at the edges of ribbons. The origin and consequence of this so-called disorder mostly occurring on PO{sub 4} configurations is intensively discussed and has been characterized by infrared spectroscopy and by neutron diffraction on similar compounds. It is noticeable that the great number of antagonist PO{sub 4} configurations may order along the b-axis within a large periodicity which involves incommensurate lattice.

OSTI ID:
20655405
Journal Information:
Journal of Solid State Chemistry, Vol. 177, Issue 11; Other Information: DOI: 10.1016/j.jssc.2004.06.057; PII: S0022-4596(04)00370-6; Copyright (c) 2004 Elsevier Science B.V., Amsterdam, The Netherlands, All rights reserved; Country of input: International Atomic Energy Agency (IAEA); ISSN 0022-4596
Country of Publication:
United States
Language:
English