51V NMR study of the kagome staircase compound Ni3V2O8

被引:10
作者
Ogloblichev, V. [1 ,2 ]
Kumagai, K. [1 ]
Verkhovskii, S. [2 ]
Yakubovsky, A. [3 ]
Mikhalev, K. [2 ]
Furukawa, Yu. [1 ]
Gerashenko, A. [2 ]
Smolnikov, A. [2 ]
Barilo, S. [4 ]
Bychkov, G. [4 ]
Shiryaev, S. [4 ]
机构
[1] Hokkaido Univ, Fac Sci, Dept Phys, Sapporo, Hokkaido 0600810, Japan
[2] Russian Acad Sci, Ural Div, Inst Met Phys, Ekaterinburg 620041, Russia
[3] Kurchatov Inst, Russian Res Ctr, Moscow 123182, Russia
[4] Inst Solid State & Semicond Phys, Minsk 220072, BELARUS
基金
俄罗斯基础研究基金会;
关键词
D O I
10.1103/PhysRevB.81.144404
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
We used V-51 NMR to study magnetic ordering in the Ni3V2O8 single crystal with a Kagome staircase structure of Ni atoms. The NMR spectra were measured in the temperature range T= (3-300) K and magnetic fields H= (2-9.4) T directed along the main a, b, c axes of the orthorhombic (Cmca) crystal. The local magnetic field at the V-51 NMR probe determines position and the shape of the corresponding NMR line. These parameters yield an unique information, respectively, on the uniform and the staggered spin components of the ordered Ni. The NMR data collected at H >= 2 T are considered in line with predictions of the representation theory [A. Harris, Phys. Rev. B 76, 054447 (2007)] with a result that incommensurate amplitude-modulated structure of the spine Ni-s spins acquires in the high-temperature incommensurate (HTI) phase two prominent nearly equal spin components S-a approximate to S-c >> S-b instead of the longitudinal incommensurate spin-density wave (SDW) order with S-a >> S-c, S-b as it was deduced from neutron-diffraction data [M. Kenzelmann et al., Phys. Rev. B 74, 014429 (2006)]. No noticeable variation of SDW polarization in the ab plane was detected below the HTI-low-temperature incommensurate (LTI) transition. In both the HTI and LTI phases two almost equal spin components of the Ni-s spins S-a approximate to S-c >> S-b exist at H < 4.7 T. Their phasing is still not determined. The bulk magnetization in these phases is explained by contribution of the cross-tie Ni-c spins which antiferromagnetic structure in the LTI phase is canted along H.
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页数:9
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