The magnetic phase diagram of the HoCo2X2 (X = Ge, Si) and DyCo2Ge2 compounds by neutron diffraction

被引:8
作者
Schobinger-Papamantellos, P
Buschow, KHJ
Ritter, C
Keller, L
机构
[1] ETH Zentrum, Lab Kristallog, CH-8092 Zurich, Switzerland
[2] Univ Amsterdam, Van Waals Zeeman Inst, NL-1018 XE Amsterdam, Netherlands
[3] Inst Laue Langevin, F-38042 Grenoble, France
[4] ETH Zuerich, Neutron Scattering Lab, CH-5232 Villigen, Switzerland
[5] PSI, CH-5232 Villigen, Switzerland
关键词
rare-earth cobalt germanide; neutron diffraction; magnetic structure; RARE-EARTH COMPOUNDS; PRCO2SI2; PRCO2GE2; TM;
D O I
10.1016/S0304-8853(03)00176-8
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
The magnetic ordering of the tetragonal (14/mmm) HoCo2X2 (X=Ge, Si) and DyCo2Ge2 compounds with the ThCr2Si2 type of structure has been reinvestigated by neutron powder diffraction. The HoCo2Si2 compound orders exclusively with the type-I antiferromagnetic structure with the wave vector q = (0, 0, 1) and the moments confined to the c-axis, while the magnetic-phase diagrams of the DyCo2Ge2 and HoCo2Ge2 compounds comprise three distinct regions of magnetic ordering: a low-temperature structure also of type-I (q, = (0, 0, 1)), stable in the range between 2 K and T-1C, a high-temperature longitudinal sine wave modulated structure with the wave vector q(2) = (0,0, 1 - q(z)), stable in the range T-IC-T-N and a coexistence region of q(1) and q(2) around T-IC. The wave vector component q(z) has a temperature-dependent length and locks-in by a first-order transition to the value q(z) = 0 at T-IC. In the case of the DyCo2Ge2 compound a spin reorientation transition was detected in the low-temperature range. The ordered moment values at 1.5 K are 7.8(1) mu(B)/Dy and 9.33(1) mu(B)/Ho for the RCo2Ge2 compounds and 8.8(1) mu(B)/Ho atom for the HoCo2Si2 compound at 3 K. (C) 2003 Elsevier Science B.V. All rights reserved.
引用
收藏
页码:130 / 141
页数:12
相关论文
共 26 条
[1]  
DUONG NP, 2002, THESIS U AMSTERDAM
[2]  
Gignoux D., 1997, Handbook of Magnetic Materials, V10, P239
[3]   Molecular field calculations of the phase transitions in NdCo2Si2 [J].
Hattori, K ;
Chen, CF ;
Sakamoto, M ;
Shigeoka, T ;
Iwata, N .
PHYSICA B, 1998, 252 (1-2) :76-80
[4]   Effects of band filling on magnetic structures:: The case of RNi2Ge2 [J].
Islam, Z ;
Detlefs, C ;
Song, C ;
Goldman, AI ;
Antropov, V ;
Harmon, BN ;
Bud'ko, SL ;
Wiener, T ;
Canfield, PC ;
Wermeille, D ;
Finkelstein, KD .
PHYSICAL REVIEW LETTERS, 1999, 83 (14) :2817-2820
[5]   Neutron diffraction and x-ray resonant exchange-scattering studies of the zero-field magnetic structures of TbNi2Ge2 [J].
Islam, Z ;
Detlefs, C ;
Goldman, AI ;
Bud'ko, SL ;
Canfiield, PC ;
Hili, JP ;
Gibbs, D ;
Vogt, T ;
Zheludev, A .
PHYSICAL REVIEW B, 1998, 58 (13) :8522-8533
[6]   Magnetic phase diagram of PrCo2Si2 with long period commensurate structure [J].
Kawae, T ;
Mito, M ;
Hitaka, M ;
Ichikawa, F ;
Shigeoka, T ;
Iwata, N ;
Takeda, K .
JOURNAL OF THE PHYSICAL SOCIETY OF JAPAN, 2000, 69 (02) :586-591
[7]   NEUTRON-DIFFRACTION STUDY OF RECO2SI2 INTERMETALLICS [J].
LECIEJEWICZ, J ;
KOLENDA, M ;
SZYTULA, A .
SOLID STATE COMMUNICATIONS, 1983, 45 (02) :145-148
[8]   A MAGNETIC PHASE-TRANSITION IN UCU2GE2 [J].
LECIEJEWICZ, J ;
CHELMICKI, L .
SOLID STATE COMMUNICATIONS, 1982, 41 (02) :167-168
[9]  
LECIEJEWICZ J, 1981, P INT C CRYST EL FIE, P327
[10]   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