STRUCTURAL-PROPERTIES OF A NOVEL MAGNETIC TERNARY PHASE - ND3(FE1-XTIX)29 (0.04-LESS-THAN-OR-EQUAL-TO-X-LESS-THAN-OR-EQUAL-TO-0.06)

被引:161
作者
LI, HS
CADOGAN, JM
DAVIS, RL
MARGARIAN, A
DUNLOP, JB
机构
[1] AUSTRALIAN NUCL SCI & TECHNOL ORG,SUTHERLAND,NSW 2234,AUSTRALIA
[2] UNIV TECHNOL SYDNEY,DEPT APPL PHYS,BROADWAY,NSW 2007,AUSTRALIA
[3] CSIRO,DIV APPL PHYS,LINDFIELD,NSW 2070,AUSTRALIA
基金
澳大利亚研究理事会;
关键词
D O I
10.1016/0038-1098(94)90051-5
中图分类号
O469 [凝聚态物理学];
学科分类号
070205 ;
摘要
A structural determination of the new magnetic ternary rare-earth iron-rich intermetallic Nd3(Fe1-xTix)29 phase, previously reported as Nd2(Fe1-xTix)19, has been carried out by means of powder X-ray diffraction on a Nd3(Fe0.955Ti0.0045)29 sample. The structure is monoclinic with the space group P2(1)/c (No.14). There are two Nd sites, namely 2a and 4e, and fifteen Fe(Ti) sites in the structure, one 2d and fourteen 4e sites. The refined lattice parameters are a = 10.641(1) angstrom, b = 8.5913(8) angstrom, c = 9.748(1) angstrom and beta = 96.928(6)-degrees, and Z = 2. The structure is a new intermediate structure between the well known rhombohedral Th2Zn17 and tetragonal ThMn12 structures. All these three structures are derived by the replacement of a fraction of the Ca(Tb or Nd) atoms in the CaCu5 structure by a pair of Cu(Zn, Fe(Ti) or Mn) atoms (dumb-bells) along the c-axis of the CaCu5 structure. The relationship between these three structures will be discussed in terms of the dumbbell substitution sequence in the hexagonal CaCu5 structure. The fractions of dumbbell replacement are 1/3, 2/5 and 1/2 for the Th2Zn17, Nd3(Fe1-xTix)29 and ThMn12 structures, respectively. It has been shown that only light rare-earths and Gd form the new Nd3(Fe1-xTix)29 phase, while for heavy rare-earths beyond Tb there should exist another new structure type.
引用
收藏
页码:487 / 492
页数:6
相关论文
共 31 条
[1]   MAGNETIC-PROPERTIES OF TERNARY FE-RICH RARE-EARTH INTERMETALLIC COMPOUNDS [J].
BUSCHOW, KHJ ;
DEMOOIJ, DB ;
BROUHA, M ;
SMIT, HHA ;
THIEL, RC .
IEEE TRANSACTIONS ON MAGNETICS, 1988, 24 (02) :1611-1616
[2]   COMPOSITION AND CRYSTAL STRUCTURE OF HEXAGONAL CU-RICH RARE EARTH-COPPER COMPOUNDS [J].
BUSCHOW, KHJ ;
VANDERGO.AS .
ACTA CRYSTALLOGRAPHICA SECTION B-STRUCTURAL CRYSTALLOGRAPHY AND CRYSTAL CHEMISTRY, 1971, B 27 (JUN15) :1085-&
[3]   MAGNETIC-PROPERTIES OF A METASTABLE SM-FE PHASE SYNTHESIZED BY SELECTIVELY THERMALIZED SPUTTERING [J].
CADIEU, FJ ;
CHEUNG, TD ;
WICKRAMASEKARA, L ;
ALY, SH .
JOURNAL OF APPLIED PHYSICS, 1984, 55 (06) :2611-2613
[4]  
CADOGAN JM, IN PRESS J APPL PHYS
[5]  
COLLOCOTT SJ, 1992, 7TH P INT S MAGN AN, P437
[6]   PHASE-ANALYSIS BY X-RAY AND MOSSBAUER-SPECTROSCOPY OF MELT-SPUN AND SUBSEQUENTLY ANNEALED SM-(FE, CO OR NI)-TI [J].
DING, J ;
ROSENBERG, M .
JOURNAL OF THE LESS-COMMON METALS, 1990, 166 (02) :303-311
[7]  
FUERST CD, UNPUB J MAGN MAGN MA
[8]   X-RAY AND NEUTRON DETERMINATION OF A SO-CALLED TH2NI17-TYPE STRUCTURE IN LUTETIUM-IRON SYSTEM [J].
GIVORD, D ;
ROUDAUT, E ;
MOREAU, JM ;
LEMAIRE, R .
JOURNAL OF THE LESS-COMMON METALS, 1972, 29 (04) :361-&
[9]  
GIVORD D, 1972, J LESS-COMMON MET, V29, P38
[10]   HARD MAGNETIC-PROPERTIES OF R-FE-TI ALLOYS [J].
HADJIPANAYIS, GC ;
ALY, SH ;
CHEN, SF .
APPLIED PHYSICS LETTERS, 1987, 51 (24) :2048-2050