The crystal structures of R3CuGeS7 (R = Ce-Nd, Sm, Gd-Dy and Er)

被引:25
|
作者
Gulay, L. D.
Lychmanyuk, O. S.
Wolcyrz, M.
Pietraszko, A.
Olekseyuk, I. D.
机构
[1] Polish Acad Sci, Inst Low Temp & Struct Res, PL-50950 Wroclaw, Poland
[2] Volyn State Univ, Dept Gen & Inorgan Chem, UA-43009 Lutsk, Ukraine
[3] Polish Acad Sci, Inst Low Temp & Struct Res, PL-50950 Wroclaw, Poland
关键词
chalcogenides; rare earth compounds; crystal structure;
D O I
10.1016/j.jallcom.2006.01.056
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
Crystal structures of R3CuGeS7 (R = Ce, Pr, Nd, Sm, Gd, Tb, Dy and Er) (La3CuSiS7 structure type, space group P6(3), Pearson symbol hP24) were determined by means of X-ray single crystal diffraction (a = 1.0225(1) nm, c = 0.58350(7) nm, R-l = 0.0213 for Ce3CuGeS7; a = 1.0168(1)nm, c = 0.58223(7)nm, R-l =0.0284 for Pr3CuGeS7; a = 1.0123(1)nm, c = 0.57942(7)nm, R-l = 0.0240 for Nd3CuGeS7) and X-ray powder diffraction (a = 1.00144(1)nm, c = 0.57714(1)nm, R-Bragg = 0.0968 for SM3CuGeS7; a = 0.99428(1)nm, c = 0.57592(1)nm, R-Bragg = 0.0863 for Gd3CuGeS7; a = 0.98863(l) nm, c = 0.57535(l) nm, R-Bragg = 0.0838 for Tb3CuGeS7; a = 0.98371(3) nm, c = 0.57552(3) nm, R-Bragg = 0.0802 for DY3CuGeS7; a = 0.97415(l) nm, c = 0.57835(l) nm, R-Bragg = 0.0709 for Er3CuGeS7). The structures are built up from three-dimensional network of RS8 distorted square antiprisms sharing edges, consolidated by GeS4 tetrahedra and CuS3 triangles sharing edges with the antiprisms. (c) 2006 Elsevier B.V. All rights reserved.
引用
收藏
页码:159 / 163
页数:5
相关论文
共 50 条
  • [31] Crystal structure of RNiPb (R = Y, Nd, Sm, Gd, Tb, Dy, Ho, Er, Tm, Lu) compounds
    Gulay, L.D., 1600, Elsevier Sequoia SA, Lausanne, Switzerland (313): : 1 - 2
  • [32] THE CRYSTAL-STRUCTURE OF THE COMPOUNDS R8GA3CO (R=CE, PR, ND, SM, TB, DY, HO, ER, TM)
    GRIN, YN
    SICHEVICH, OM
    GLADYSHEVSKY, RE
    YARMOLYUK, YP
    KRISTALLOGRAFIYA, 1984, 29 (04): : 708 - 711
  • [33] THE CRYSTAL-STRUCTURE OF RGACO (R=PR, ND, SM, GD, TB, DY, HO, ER, Y) COMPOUNDS
    SICHEVICH, OM
    GLADYSHEVSKY, RE
    GRYN, YN
    YARMOLYUK, YP
    DOPOVIDI AKADEMII NAUK UKRAINSKOI RSR SERIYA B-GEOLOGICHNI KHIMICHNI TA BIOLOGICHNI NAUKI, 1982, (11): : 57 - 59
  • [34] Magnetic ordering of novel La3NiGe2-type R3CoGe2 compounds (R = Pr, Nd, Sm, Gd-Dy)
    Manfrinetti, P.
    Morozkin, A. V.
    Isnard, O.
    Wrubl, F.
    Mozharivskyj, Yu.
    Svitlyk, V.
    INTERMETALLICS, 2011, 19 (03) : 321 - 326
  • [35] Preparation of a single phase R3(Fe,Mo)29 (R = Ce, Nd, Sm, Gd, Tb, Dy and Y)
    Pan, HG
    Chen, WX
    Chen, Y
    Chen, CP
    TRANSACTIONS OF NONFERROUS METALS SOCIETY OF CHINA, 1998, 8 (03) : 392 - 396
  • [37] Preparation of single phase R3 (Fe, Mo)29 (R=Ce, Nd, Sm, Gd, Tb, Dy and Y)
    Zhejiang Univ, Hangzhou, China
    Trans Nonferrous Met Soc China, 3 (392-396):
  • [38] Crystal structures of double vanadates, Ca9R(VO4)7.: III.: R = Nd, Sm, Gd, or Ce
    Belik, AA
    Morozov, VA
    Grechkin, SV
    Khasanov, SS
    Lazoryak, BI
    CRYSTALLOGRAPHY REPORTS, 2000, 45 (05) : 728 - 733
  • [39] Magnetic properties of R2AgIn3 compounds (R=Ce, Pr, Nd, Gd, Tb, Dy, Ho, Er)
    Siouris, IM
    Semitelou, IP
    Yakinthos, JK
    Schmitt, D
    EUROPEAN POWDER DIFFRACTION, PTS 1 AND 2, 2000, 321-3 : 616 - 620
  • [40] Physical properties of single crystalline RMg2Cu9 (R = Y, Ce-Nd, Gd-Dy, Yb) and the search for in-plane magnetic anisotropy in hexagonal systems
    Kong, Tai
    Meier, William R.
    Lin, Qisheng
    Saunders, Scott M.
    Bud'ko, Sergey L.
    Flint, Rebecca
    Canfield, Paul C.
    PHYSICAL REVIEW B, 2016, 94 (14)