Crystal structure and magnetic properties of R3Co0.5GeS7 (R = Y, La, Ce, Pr, Nd, Sm, Gd, Tb, Dy, Ho, Er and Tm) and R3Ni0.5GeS7 (R = Y, Ce, Sm, Gd, Tb, Dy, Ho, Er and Tm)

被引:19
|
作者
Daszkiewicz, M. [1 ]
Pashynska, Yu. O. [2 ]
Marchuk, O. V. [3 ]
Gulay, L. D. [4 ]
Kaczorowski, D. [1 ]
机构
[1] Polish Acad Sci, Inst Low Temp & Struct Res, PL-50950 Wroclaw, Poland
[2] Lutsk Natl Tech Univ, Dept Mat Sci, UA-43018 Lutsk, Ukraine
[3] Eastern European Natl Univ, Dept Inorgan & Phys Chem, UA-43009 Lutsk, Ukraine
[4] Eastern European Natl Univ, Dept Ecol & Protect Environm, UA-43009 Lutsk, Ukraine
关键词
Rare earth compounds; Chalcogenides; Crystal structures; X-ray single crystal diffraction; Magnetic properties;
D O I
10.1016/j.jallcom.2015.06.059
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
The crystal structure of quaternary compounds R3Co0.5GeS7 (R = Y, La, Ce, Pr, Nd, Sm, Gd, Tb, Dy, Ho, Er and Tm) and R3Ni0.5GeS7 (R = Y, Ce, Sm, Gd, Tb, Dy, Ho, Er and Tm) (La3Mn0.5SiS7 structure type, space group P6(3), Pearson symbol hP23) was determined by means of X-ray single crystal diffraction. The R atoms are located in trigonal prisms with two additional atoms, the Co (Ni) atoms occupy octahedra, the Ge atoms are located in tetrahedra. Magnetic properties of the compounds R3Co0.5GeS7 (R = Sm and Gd) and R3Ni0.5GeS7 (R = Gd, Dy, Er and Tm) were studied down to 1.72 K. Their magnetic behaviour is governed by trivalent rare-earth and divalent transition-metal constituents. In each material, the magnetic exchange interactions are dominated by antiferromagnetic correlations, which promote long-range magnetic orderings at low temperatures. (C) 2015 Elsevier B.V. All rights reserved.
引用
收藏
页码:445 / 455
页数:11
相关论文
共 50 条
  • [41] Structure and Magnetic Properties of RIn2.9Co0.1 (R = La, Ce, Pr, Nd, Gd, Tb, Dy, Ho, Er, Tm, Lu)
    Tan, Hui
    Guo, Yong-Quan
    CRYSTAL RESEARCH AND TECHNOLOGY, 2019, 54 (08)
  • [42] Physical properties of ternary compounds R2Ni2Pb (R = Y, Sm, Gd, Tb, Dy, Ho, Er and Tm)
    Gulay, LD
    Hiebl, K
    JOURNAL OF ALLOYS AND COMPOUNDS, 2003, 351 (1-2) : 35 - 39
  • [43] MAGNETIC PROPERTIES OF RCO2 GE2 COMPOUNDS (R = LA, CE, PR, ND, SM, GD, TB, DY, HO, ER, TM, YB, LU, AND Y)
    MCCALL, WM
    NARASIMHAN, KS
    BUTERA, RA
    JOURNAL OF APPLIED PHYSICS, 1973, 44 (10) : 4724 - 4726
  • [44] Crystal structure of R6Co2+xPb1-y (R=Y, Gd, Tb, Dy, Ho, Er, Tm, Lu) and R6Ni2+xPb1-y (R=Tb, Dy, Ho, Er, Tm, Lu) compounds
    Gulay, LD
    Wolcyrz, M
    JOURNAL OF ALLOYS AND COMPOUNDS, 2001, 315 (1-2) : 164 - 168
  • [45] THE CRYSTAL-STRUCTURE OF RNI9IN2 (R=Y, LA, CE, PR, ND, SM, EU, GD, TB, DY, HO, ER) COMPOUNDS
    KALYCHAK, YM
    AKSELRUD, LG
    ZAREMBA, VI
    BARANYAK, VM
    DOPOVIDI AKADEMII NAUK UKRAINSKOI RSR SERIYA B-GEOLOGICHNI KHIMICHNI TA BIOLOGICHNI NAUKI, 1984, (08): : 35 - 37
  • [46] MAGNETIC-PROPERTIES OF R(3)CO (R=GD, TB, DY, HO, ER)
    NAGAI, H
    OGIWARA, F
    AMAKO, Y
    YOSHIE, H
    KOGA, K
    ADACHI, K
    JOURNAL OF MAGNETISM AND MAGNETIC MATERIALS, 1995, 140 : 793 - 794
  • [47] Crystal structures of the R3CuSnSe7 (R = La, Ce, Pr, Nd, Sm, Gd, Tb and Dy) compounds
    Gulay, LD
    Olekseyuk, ID
    JOURNAL OF ALLOYS AND COMPOUNDS, 2005, 388 (02) : 274 - 278
  • [48] INTRINSIC MAGNETIC-PROPERTIES OF RFE(10)MO(2) COMPOUNDS (R=Y, PR, ND, SM, GD, TB, DY, HO, ER, OR TM)
    KOU, XC
    GROSSINGER, R
    WIESINGER, G
    LIU, JP
    DEBOER, FR
    KLEINSCHROTH, I
    KRONMULLER, H
    PHYSICAL REVIEW B, 1995, 51 (13) : 8254 - 8265
  • [49] AC-SUSCEPTIBILITY ANOMALY AND MAGNETIC-ANISOTROPY OF R2CO17 COMPOUNDS, WITH R = Y, CE, PR, ND, SM, GD, TB, DY, HO, ER, TM, AND LU
    KOU, XC
    ZHAO, TS
    GROSSINGER, R
    DEBOER, FR
    PHYSICAL REVIEW B, 1992, 46 (10): : 6225 - 6235
  • [50] Crystal structure and magnetic properties of novel La(Ce, Pr)R′PbSi2S8 (R′ = Ce, Pr, Sm, Tb, Dy, Y, Ho and Er) compounds
    Kaczorowski, D.
    Melnychuk, Kh O.
    Marchuk, O., V
    Gulay, L. D.
    Daszkiewicz, M.
    JOURNAL OF SOLID STATE CHEMISTRY, 2020, 290