TY - JOUR
T1 - Magnetic structures and quadratic magnetoelectric effect in LiNiPO4 beyond 30 T
AU - Fogh, Ellen
AU - Kihara, Takumi
AU - Toft-Petersen, Rasmus
AU - Bartkowiak, Maciej
AU - Narumi, Yasuo
AU - Prokhnenko, Oleksandr
AU - Miyake, Atsushi
AU - Tokunaga, Masashi
AU - Oikawa, Kenichi
AU - Sørensen, Michael Korning
AU - Dyrnum, Julia Cathrine
AU - Grimmer, Hans
AU - Nojiri, Hiroyuki
AU - Christensen, Niels Bech
PY - 2020
Y1 - 2020
N2 - Neutron diffraction with static and pulsed magnetic fields is used to directly probe the magnetic structures in LiNiPO4 up to 25 T and 42 T, respectively. By combining these results with magnetometry and electric polarization measurements under pulsed fields, the magnetic and magnetoelectric phases are investigated up to 56 T applied along the easy c axis. In addition to the already known transitions at lower fields, three new ones are reported at 37.6, 39.4, and 54 T. Ordering vectors are identified with QVI = (0, 1/3, 0) in the interval 37.6 - 39.4 T and QVII = (0, 0, 0) in the interval 39.4 - 54 T. A quadratic magnetoelectric effect is discovered in the QVII = (0, 0, 0) phase and the field dependence of the induced electric polarization is described using a simple mean-field model. The observed magnetic structure and magnetoelectric tensor elements point to a change in the lattice symmetry in this phase. We speculate on the possible physical mechanism responsible for the magnetoelectric effect in LiNiPO4.
AB - Neutron diffraction with static and pulsed magnetic fields is used to directly probe the magnetic structures in LiNiPO4 up to 25 T and 42 T, respectively. By combining these results with magnetometry and electric polarization measurements under pulsed fields, the magnetic and magnetoelectric phases are investigated up to 56 T applied along the easy c axis. In addition to the already known transitions at lower fields, three new ones are reported at 37.6, 39.4, and 54 T. Ordering vectors are identified with QVI = (0, 1/3, 0) in the interval 37.6 - 39.4 T and QVII = (0, 0, 0) in the interval 39.4 - 54 T. A quadratic magnetoelectric effect is discovered in the QVII = (0, 0, 0) phase and the field dependence of the induced electric polarization is described using a simple mean-field model. The observed magnetic structure and magnetoelectric tensor elements point to a change in the lattice symmetry in this phase. We speculate on the possible physical mechanism responsible for the magnetoelectric effect in LiNiPO4.
U2 - 10.1103/physrevb.101.024403
DO - 10.1103/physrevb.101.024403
M3 - Journal article
SN - 2469-9950
VL - 101
JO - Physical Review B
JF - Physical Review B
IS - 2
M1 - 024403
ER -