TY - JOUR
T1 - Spin structures with frustrated moments in RNiAl intermetallic compounds
AU - Ehlers, G.
AU - Maletta, H.
PY - 1997/12
Y1 - 1997/12
N2 - Magnetic order in the ternary equiatomic intermetallic compounds PrNiAl, DyNiAl and HoNiAl is investigated by means of neutron powder diffraction and dc- and ac-susceptibility measurements. DyNiAl shows two magnetic phases: It is ferromagnetic between T1 = 15 K and Tc = 31 K and a tilted antiferromagnet below T1. HoNiAl is a ferromagnet in a narrow temperature region just below Tc = 14.5 K, but furthermore exhibits two tilted antiferromagnetic phases (T1 = 5.5 K, T2 = 12.5 K). The corresponding magnetic structures differ in the ordering of some of the magnetic moments which are coupled by frustrated bonds. The existence of those frustrated moments, which is induced by the topology is a common phenomenon in the hexagonal RNiAl series. They are manifested with reduced mean values of their moments in the elastic neutron spectra. Another interesting observation is the scaling of the second temperature T1 at which the frustrated spins change their order: For all heavy rare earths investigated so far (R = Tb, Dy, Ho) we find T1:TN,C≈1:2. PrNiAl displays an incommensurate sinusoidal (TSW) structure with XY spin behaviour below TN = 6.9 K, and only one ordered phase is found. The observed ordering temperatures roughly follow the de Gennes scaling factor.
AB - Magnetic order in the ternary equiatomic intermetallic compounds PrNiAl, DyNiAl and HoNiAl is investigated by means of neutron powder diffraction and dc- and ac-susceptibility measurements. DyNiAl shows two magnetic phases: It is ferromagnetic between T1 = 15 K and Tc = 31 K and a tilted antiferromagnet below T1. HoNiAl is a ferromagnet in a narrow temperature region just below Tc = 14.5 K, but furthermore exhibits two tilted antiferromagnetic phases (T1 = 5.5 K, T2 = 12.5 K). The corresponding magnetic structures differ in the ordering of some of the magnetic moments which are coupled by frustrated bonds. The existence of those frustrated moments, which is induced by the topology is a common phenomenon in the hexagonal RNiAl series. They are manifested with reduced mean values of their moments in the elastic neutron spectra. Another interesting observation is the scaling of the second temperature T1 at which the frustrated spins change their order: For all heavy rare earths investigated so far (R = Tb, Dy, Ho) we find T1:TN,C≈1:2. PrNiAl displays an incommensurate sinusoidal (TSW) structure with XY spin behaviour below TN = 6.9 K, and only one ordered phase is found. The observed ordering temperatures roughly follow the de Gennes scaling factor.
UR - http://www.scopus.com/inward/record.url?scp=0007813042&partnerID=8YFLogxK
U2 - 10.1007/s002570050215
DO - 10.1007/s002570050215
M3 - Article
AN - SCOPUS:0007813042
SN - 0722-3277
VL - 101
SP - 317
EP - 327
JO - Zeitschrift für Physik B Condensed Matter
JF - Zeitschrift für Physik B Condensed Matter
IS - 3
ER -