TY - JOUR
T1 - Field dependence of magnetic ordering in Kagomé-staircase compound Ni3 V2 O8
AU - Kenzelmann, M.
AU - Harris, A. B.
AU - Aharony, A.
AU - Entin-Wohlman, O.
AU - Yildirim, T.
AU - Huang, Q.
AU - Park, S.
AU - Lawes, G.
AU - Broholm, C.
AU - Rogado, N.
AU - Cava, R. J.
AU - Kim, K. H.
AU - Jorge, G.
AU - Ramirez, A. P.
PY - 2006/8/1
Y1 - 2006/8/1
N2 - We present powder and single-crystal neutron diffraction and bulk measurements of the Kagomé-staircase compound Ni3 V2 O8 (NVO) in fields up to 8.5 T applied along the c direction. (The Kagomé plane is the a-c plane.) This system contains two types of Ni ions, which we call "spine" and "cross-tie." Our neutron measurements can be described with the paramagnetic space group Cmca for T<15 K and each observed magnetically ordered phase is characterized by the appropriate irreducible representation(s). Our zero-field measurements show that at TPH =9.1 K NVO undergoes a transition to a predominantly longitudinal incommensurate structure in which the spine spins are nearly along the a -axis. At THL =6.3 K, there is a transition to an elliptically polarized incommensurate structure with both spine and cross-tie moments in the a-b plane. At TLC =4 K the system undergoes a first-order phase transition to a commensurate antiferromagnetic structure with the staggered magnetization primarily along the a -axis and a weak ferromagnetic moment along the c -axis. A specific heat anomaly at T CC′ =2.3 K indicates an additional transition, which remarkably does not affect Bragg peaks of the commensurate C structure. Neutron, specific heat, and magnetization measurements produce a comprehensive temperature-field phase diagram. The symmetries of the incommensurate magnetic phases are consistent with the observation that only one phase is electrically polarized. The magnetic structures are explained theoretically using a simplified model Hamiltonian, that involves competing nearest- and next-nearest-neighbor exchange interactions, single-ion anisotropy, pseudodipolar interactions, and Dzyaloshinskii-Moriya interactions.
AB - We present powder and single-crystal neutron diffraction and bulk measurements of the Kagomé-staircase compound Ni3 V2 O8 (NVO) in fields up to 8.5 T applied along the c direction. (The Kagomé plane is the a-c plane.) This system contains two types of Ni ions, which we call "spine" and "cross-tie." Our neutron measurements can be described with the paramagnetic space group Cmca for T<15 K and each observed magnetically ordered phase is characterized by the appropriate irreducible representation(s). Our zero-field measurements show that at TPH =9.1 K NVO undergoes a transition to a predominantly longitudinal incommensurate structure in which the spine spins are nearly along the a -axis. At THL =6.3 K, there is a transition to an elliptically polarized incommensurate structure with both spine and cross-tie moments in the a-b plane. At TLC =4 K the system undergoes a first-order phase transition to a commensurate antiferromagnetic structure with the staggered magnetization primarily along the a -axis and a weak ferromagnetic moment along the c -axis. A specific heat anomaly at T CC′ =2.3 K indicates an additional transition, which remarkably does not affect Bragg peaks of the commensurate C structure. Neutron, specific heat, and magnetization measurements produce a comprehensive temperature-field phase diagram. The symmetries of the incommensurate magnetic phases are consistent with the observation that only one phase is electrically polarized. The magnetic structures are explained theoretically using a simplified model Hamiltonian, that involves competing nearest- and next-nearest-neighbor exchange interactions, single-ion anisotropy, pseudodipolar interactions, and Dzyaloshinskii-Moriya interactions.
UR - http://www.scopus.com/inward/record.url?scp=33746442108&partnerID=8YFLogxK
U2 - 10.1103/PhysRevB.74.014429
DO - 10.1103/PhysRevB.74.014429
M3 - Article
AN - SCOPUS:33746442108
SN - 1098-0121
VL - 74
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 1
M1 - 014429
ER -