TY - JOUR
T1 - Tbx Er1-x Ni5 compounds
T2 - An ideal model system for competing Ising- XY anisotropy energies
AU - Pirogov, A. N.
AU - Park, J. G.
AU - Ermolenko, A. S.
AU - Korolev, A. V.
AU - Kuchin, A. G.
AU - Lee, Seongsu
AU - Choi, Y. N.
AU - Park, Junghwan
AU - Ranot, Mahipal
AU - Yi, Junghwan
AU - Gerasimov, E. G.
AU - Dorofeev, Yu A.
AU - Vokhmyanin, A. P.
AU - Podlesnyak, A. A.
AU - Swainson, I. P.
PY - 2009/5/1
Y1 - 2009/5/1
N2 - We have studied Tbx Er1-x Ni5 (x=0, 0.1, 0.2, 0.3, 0.4, 0.6, 0.8, 0.925, and 1.0) compounds by using several experimental techniques such as ac-susceptibility, heat-capacity, and neutron-diffraction measurements. All the compounds are found to crystallize in the CaCu5 -type structure with space group P6/mmm. The a axis shows a linear increase with Tb concentration, whereas the c axis remains almost unchanged over the whole doping range. Our neutron-diffraction studies revealed that samples for 0≤x≤0.8 have a commensurate magnetic structure with k=0, whereas the two samples on the Tb-rich phase (x=0.925 and 1.0) have an incommensurate structure. Of particular interest is that individual Tb and Er moments keep their mutually orthogonal arrangement seen at the end-member compositions over the whole doping range, due to very strong magnetic anisotropy of single-ion nature. We have established a complete magnetic x-T phase diagram of Tbx Er1-x Ni5 to find that two straight lines of the ordering of the Tb and Er subsystems are persistently seen, which intersect at a tetracritical point.
AB - We have studied Tbx Er1-x Ni5 (x=0, 0.1, 0.2, 0.3, 0.4, 0.6, 0.8, 0.925, and 1.0) compounds by using several experimental techniques such as ac-susceptibility, heat-capacity, and neutron-diffraction measurements. All the compounds are found to crystallize in the CaCu5 -type structure with space group P6/mmm. The a axis shows a linear increase with Tb concentration, whereas the c axis remains almost unchanged over the whole doping range. Our neutron-diffraction studies revealed that samples for 0≤x≤0.8 have a commensurate magnetic structure with k=0, whereas the two samples on the Tb-rich phase (x=0.925 and 1.0) have an incommensurate structure. Of particular interest is that individual Tb and Er moments keep their mutually orthogonal arrangement seen at the end-member compositions over the whole doping range, due to very strong magnetic anisotropy of single-ion nature. We have established a complete magnetic x-T phase diagram of Tbx Er1-x Ni5 to find that two straight lines of the ordering of the Tb and Er subsystems are persistently seen, which intersect at a tetracritical point.
UR - https://www.scopus.com/pages/publications/66849111743
U2 - 10.1103/PhysRevB.79.174412
DO - 10.1103/PhysRevB.79.174412
M3 - Article
AN - SCOPUS:66849111743
SN - 1098-0121
VL - 79
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 17
M1 - 174412
ER -