Published December 1, 2010 | Version v1
Journal article

Structural and magnetic properties of LiMn1.5Fe0.5O4 spinel oxide

  • 1. Department of Physics, University of Science and Technology Beijing, Beijing 100083 (China)
  • 2. Department of Engineering Science and Materials, University of Puerto Rico at Mayaguez, Mayagues, PR 00681-9044 (Puerto Rico)
  • 3. Department of Physics, Capital Normal University, Beijing 100037 (China)
  • 4. School of Material Science and Engineering, University of Science and Technology Beijing, Beijing 100083 (China)
  • 5. National High Magnetic Field Laboratory, Florida State University, 1800 E. Paul Dirac Drive, Tallahassee, FL 32310-3706 (United States)
  • 6. Department of Physics, University of Texas at Arlington, Arlington, TX 76019 (United States)
  • 7. Department of Engineering Science and Materials, University of Puerto Rico at Mayaguez, Mayagues, PR 00681-9044 (United States)
  • 8. Department of Physics, University of Puerto Rico at Mayaguez, Mayagues, PR 00681 (Puerto Rico)

Description

Geometrical frustration, which arises from the topology of a well-ordered structure rather than from disorder, has recently become a renewed interest. In particular, geometrical frustration among spins in the spinel oxides can lead to exotic low-temperature states. We reported a joint experimental and theoretical investigation of Fe-doping effect on LiMn2O4 spinel oxide in which magnetic moments have geometrical frustration. The structural and physical properties of LiMn1.5Fe0.5O4 were studied by means of Moessbauer spectroscopy, X-ray diffraction, scanning electron microscope (SEM), electrical and magnetic measurements. Electronic conductivity measurements showed that Verwey-type transition is absent in heavily Fe-doped LiMn2O4. In addition, LiMn1.5Fe0.5O4 exhibits a semiconductor characteristic in resistivity with an energy gap Eg=0.27 eV, which is consistent with our first-principle simulation. A large resistivity at room temperature for LiMn1.5Fe0.5O4 indicates low concentration of conduction electrons corresponding to electronic localization behavior. X-ray diffraction refinement as well as Moessbauer analysis suggests that Fe ions preferentially substitute for Mn ions on the octahedral B-sites. Moreover, small amount of Fe replace for Li ions to form a site inversion in spinel structure. In contrast to the pure and low-Fe-doped LiMn2O4 samples, LiMn1.5Fe0.5O4 has an antiferromagnetic transition at TN=34 K. The Fe dopants enhance the antiferromagnetic interaction among moments accompanied by breaking the original moment equilibrium and suppressing the magnetic frustration in LiMn2O4.

Availability note (English)

Available from http://dx.doi.org/10.1016/j.physb.2010.08.050

Additional details

Identifiers

DOI
10.1016/j.physb.2010.08.050;
PII
S0921-4526(10)00820-3;

Publishing Information

Journal Title
Physica. B, Condensed Matter
Journal Volume
405
Journal Issue
23
Journal Page Range
p. 4733-4739
ISSN
0921-4526
CODEN
PHYBE3

Optional Information

Copyright
Copyright (c) 2010 Elsevier Science B.V., Amsterdam, The Netherlands, All rights reserved.