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Phys. Rev. B 79, 174435 (2009) [7 pages]

Tweaking the spin-wave dispersion and suppressing the incommensurate phase in LiNiPO4 by iron substitution

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Jiying Li1,2,3, Thomas B. S. Jensen4, Niels H. Andersen4, Jerel L. Zarestky1, R. William McCallum5, Jae-Ho Chung6, Jeffrey W. Lynn2, and David Vaknin1,*
1Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA
2NIST Center for Neutron Research, National Institute of Standards and Technology, Gaithersburg, Maryland 20899, USA
3Department of Materials Science and Engineering, University of Maryland, College Park, Maryland 20742, USA
4Materials Research Division, Risø DTU, Technical University of Denmark, DK-4000 Roskilde, Denmark
5Ames Laboratory and Department of Materials Science and Engineering, Iowa State University, Ames, Iowa 50011, USA
6Department of Physics, Korea University, Seoul 136-713, Korea

Received 18 March 2009; published 29 May 2009

Elastic and inelastic neutron-scattering studies of Li(Ni1−xFex)PO4 single crystals reveal anomalous spin-wave dispersions along the crystallographic direction parallel to the characteristic wave vector of the magnetic incommensurate phase. The anomalous spin-wave dispersion (magnetic soft mode) indicates the instability of the Ising-type ground state that eventually evolves into the incommensurate phase as the temperature is raised. The pure LiNiPO4 system (x=0) undergoes a first-order magnetic phase transition from a long-range incommensurate phase to an antiferromagnetic (AFM) ground state at TN=20.8 K. At 20% Fe concentrations, although the AFM ground state is to a large extent preserved as that of the pure system, the phase transition is second order, and the incommensurate phase is completely suppressed. Analysis of the dispersion curves using a Heisenberg spin Hamiltonian that includes interplane and in-plane nearest- and next-nearest-neighbor couplings reveals frustration due to strong competing interactions between nearest- and next-nearest-neighbor sites, consistent with the observed incommensurate structure. The Fe substitution only slightly lowers the extent of the frustration, sufficient to suppress the incommensurate phase. An energy gap in the dispersion curves gradually decreases with the increase in Fe content from ∼2 meV for the pure system (x=0) to ∼0.9 meV for x=0.2.

© 2009 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevB.79.174435
DOI:
10.1103/PhysRevB.79.174435
PACS:
75.25.+z, 75.50.Ee, 78.20.Ls

*vaknin@ameslab.gov