TY - JOUR
T1 - Neutron diffraction study of antiferromagnetic ErNi3Ga9 in magnetic fields
AU - Ninomiya, Hiroki
AU - Sato, Takaaki
AU - Matsumoto, Yuji
AU - Moyoshi, Taketo
AU - Nakao, Akiko
AU - Ohishi, Kazuki
AU - Kousaka, Yusuke
AU - Akimitsu, Jun
AU - Inoue, Katsuya
AU - Ohara, Shigeo
N1 - Publisher Copyright:
© 2017 Elsevier B.V.
PY - 2018/5/1
Y1 - 2018/5/1
N2 - We report specific heat, magnetization, magnetoresistance, and neutron diffraction measurements of single crystals of ErNi3Ga9. This compound crystalizes in a chiral structure with space group R32. The erbium ions form a two–dimensional honeycomb structure. ErNi3Ga9 displays antiferromagnetic order below 6.4 K. We determined that the magnetic structure is slightly amplitude–modulated as well as antiferromagnetic with q=(0,0,0.5). The magnetic properties are described by an Ising–like model in which the magnetic moment is always along the c–axis owing to the large uniaxial anisotropy caused by the crystalline electric field effect in the low temperature region. When the magnetic field is applied along the c–axis, a metamagnetic transition is observed around 12 kOe at 2 K. ErNi3Ga9 possesses crystal chirality, but the antisymmetric magnetic interaction, the so-called Dzyaloshinskii–Moriya (DM) interaction, does not contribute to the magnetic structure, because the magnetic moments are parallel to the DM–vector.
AB - We report specific heat, magnetization, magnetoresistance, and neutron diffraction measurements of single crystals of ErNi3Ga9. This compound crystalizes in a chiral structure with space group R32. The erbium ions form a two–dimensional honeycomb structure. ErNi3Ga9 displays antiferromagnetic order below 6.4 K. We determined that the magnetic structure is slightly amplitude–modulated as well as antiferromagnetic with q=(0,0,0.5). The magnetic properties are described by an Ising–like model in which the magnetic moment is always along the c–axis owing to the large uniaxial anisotropy caused by the crystalline electric field effect in the low temperature region. When the magnetic field is applied along the c–axis, a metamagnetic transition is observed around 12 kOe at 2 K. ErNi3Ga9 possesses crystal chirality, but the antisymmetric magnetic interaction, the so-called Dzyaloshinskii–Moriya (DM) interaction, does not contribute to the magnetic structure, because the magnetic moments are parallel to the DM–vector.
KW - Chiral crystal
KW - DM-interaction
KW - ErNiGa
KW - Ising antiferromagnet
KW - Metamagnetism
KW - Neutron diffraction
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U2 - 10.1016/j.physb.2017.09.057
DO - 10.1016/j.physb.2017.09.057
M3 - Article
AN - SCOPUS:85029598331
SN - 0921-4526
VL - 536
SP - 392
EP - 396
JO - Physica B: Condensed Matter
JF - Physica B: Condensed Matter
ER -