Magnetic order in the TbCo6Ge6 and TbCo2Ge2 compounds:: A neutron study

被引:10
作者
Schobinger-Papamantellos, P [1 ]
Rodriguez-Carvajal, J
Buschow, KHJ
机构
[1] ETH Zurich, Lab Kristallog, CH-8092 Zurich, Switzerland
[2] Ctr Etud Saclay, Lab Leon Brillouin, CNRS, CEA, F-91191 Gif Sur Yvette, France
[3] Univ Amsterdam, Van der Waals Zeeman Inst, NL-1018 XE Amsterdam, Netherlands
关键词
rare earth cobalt germanide; neutron diffraction; magnetic structure;
D O I
10.1016/S0925-8388(98)00556-8
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
A structure determination using high-resolution neutron powder data has shown that the hexagonal compound TbCo6Ge6 (P6/mmm) has the YCo6Ge6-type structure. The R and the Gel atoms share the 1(a) (000) and the 2(e) (00z) sites while the Ge-2 and Co atoms are at 2(c) (1/3, 2/3, 0) and 3(g) (1/2, 0, 1/2), respectively. The refinement has shown that the Tb/Ge distribution is 0.36 Tb and 0.14 Ge-1 for the 1(a) site and 0.74 Gel and 0.26 Tb for the 2(e) site. This atomic distribution leads to different R-R interactions to those observed in the parent compounds TbMn6Ge6 and TbFe6Ge6. As the Co-Co interaction is very weak a possible TbCo6Ge6 ordering could be caused by the R-R interaction. However, no evidence of magnetic ordering in TbCo6Ge6 has been obtained down to 1.5 K. The coexisting tetragonal phase (14/mmm) of TbCo6Ge6 with ThCr2Si2 structure reported earlier to order antiferromagnetically at 31 K with a uniaxial moment arrangement along c and the wave vector (001) was found to undergo a magnetic phase transition at 22 K. Above this temperature the magnetic structure changes into a longitudinal sinewave incommensurate phase with the wave vector q=(0, 0, 1-q(z)), or q(z)=0.063(1) r.l.u when referring to the primitive cell. This wave vector corresponds to a 16xc cell enlargement and its length is temperature-dependent and at T(1)approximate to 22 K locks in to the (001) value. The Tb atoms related by the centering translation are coupled antiparallely over the entire ordered regime. The ordered moment value varies from 8.8(1)mu(B)/Tb atom at 1.5 K to 7.9(1) mu(B)/Tb at 22 K. The amplitude of the modulated structure is 9.3(2)mu(B) at 24 K. (C) 1998 Elsevier Science S.A.
引用
收藏
页码:83 / 89
页数:7
相关论文
共 19 条
[1]   MAGNETIC-PROPERTIES OF RARE-EARTH MANGANESE COMPOUNDS OF THE RMN6GE6 TYPE [J].
BRABERS, JHVJ ;
DUIJN, VHM ;
DEBOER, FR ;
BUSCHOW, KHJ .
JOURNAL OF ALLOYS AND COMPOUNDS, 1993, 198 (1-2) :127-132
[2]   MAGNETIC-PROPERTIES OF RCR6GE6 COMPOUNDS [J].
BRABERS, JHVJ ;
BUSCHOW, KHJ ;
DEBOER, FR .
JOURNAL OF ALLOYS AND COMPOUNDS, 1994, 205 (1-2) :77-80
[3]  
LECIEJEWICZ J, 1982, SOLID STATE COMMUN, V45, P149
[4]  
LECIEJEWICZ J, 1981, P INT C CRYST EL FIE, P327
[5]   MAGNETIC PROPERTIES OF RCO2 GE2 COMPOUNDS (R = LA, CE, PR, ND, SM, GD, TB, DY, HO, ER, TM, YB, LU, AND Y) [J].
MCCALL, WM ;
NARASIMHAN, KS ;
BUTERA, RA .
JOURNAL OF APPLIED PHYSICS, 1973, 44 (10) :4724-4726
[6]   GD-155 MOSSBAUER-EFFECT AND MAGNETIC-PROPERTIES OF TERNARY RARE-EARTH COMPOUNDS OF THE TYPE RT2GE2 (T-EQUIVALENT-TO-3D, 4D) [J].
MULDER, FM ;
THIEL, RC ;
BUSCHOW, KHJ .
JOURNAL OF ALLOYS AND COMPOUNDS, 1993, 202 :29-35
[7]  
Olenitch R.R., 1981, DOPOV AKAD NAUK UK A, VA2, P84
[8]  
PARTHE E, 1984, HDB PHYSICS CHEM RAR, V6, P113, DOI DOI 10.1016/J.JLUMIN.2007.01.024
[9]   MAGNETIC-STRUCTURE OF PRCO2GE2, A NEUTRON-DIFFRACTION STUDY [J].
PINTO, H ;
MELAMUD, M ;
GUREWITZ, E .
ACTA CRYSTALLOGRAPHICA SECTION A, 1979, 35 (JUL) :533-536
[10]  
PINTO H, 1982, NEUTRON SCATTERING 1, P315