1/3 magnetization plateau and frustrated ferrimagnetism in a sodium iron phosphite

Research output: Contribution to journalResearch articleContributedpeer-review

Contributors

  • A. N. Vasiliev - , Ural Federal University (Author)
  • O. S. Volkova - , Ural Federal University (Author)
  • E. A. Zvereva - , Lomonosov Moscow State University (Author)
  • E. A. Ovchenkov - , Lomonosov Moscow State University (Author)
  • I. Munao - , University of St Andrews (Author)
  • L. Clark - , University of St Andrews (Author)
  • P. Lightfoot - , University of St Andrews (Author)
  • E. L. Vavilova - , TUD Dresden University of Technology (Author)
  • S. Kamusella - , Chair of Solid State Physics/Electronic Properties (Author)
  • H. -H. Klauss - , Chair of Solid State Physics/Electronic Properties (Author)
  • J. Werner - , Heidelberg University  (Author)
  • C. Koo - , Heidelberg University  (Author)
  • R. Klingeler - , Heidelberg University  (Author)
  • A. A. Tsirlin - , Augsburg University (Author)

Abstract

The sodium iron phosphite NaFe3(HPO3)(2)(H2PO3)(6) is studied by ac-magnetic susceptibility, pulsed-field magnetization, specific heat, and high-frequency electron spin resonance (HF-ESR) measurements combined with Mossbauer spectroscopy and density-functional calculations. We show that this compound develops ferrimagnetic order below T-C = 9.5K and reveals a magnetization plateau at 1/3 saturation. The plateau extends to B-c similar to 8T, whereas above B-c the magnetization increases linearly until reaching saturation at B-s similar to 27 T. The Mossbauer spectroscopy reveals two magnetically nonequivalent iron sites with the 2: 1 ratio. The HF-ESR spectra are consistent with a two-sublattice ferrimagnet and additionally pinpoint weak magnetic anisotropy as well as short-range spin order that persists well above T-C. The ferrimagnetic order in the title compound is stabilized by a network of purely antiferromagnetic exchange interactions. The spin lattice comprises layers coinciding with the crystallographic (10-1) planes, with stronger couplings J(i) similar to 1.5 K within the layers and weaker couplings J(i) = 0.3-0.4K between the layers. Both intralayer and interlayer couplings are frustrated. The ensuing ferrimagnetic order arises from a subtle interplay of the frustrated but nonequivalent exchange couplings.

Details

Original languageEnglish
Article number134401
Number of pages8
JournalPhysical Review B
Volume93
Issue number13
Publication statusPublished - 1 Apr 2016
Peer-reviewedYes

External IDs

Scopus 84963549013

Keywords

Keywords

  • TRIANGULAR LATTICE, ANTIFERROMAGNET

Library keywords