Disorder and Doubleexchange Spin Dynamics in La0'7Sr0'3MnO3 and La0'7Sr0'3CoO3 from NMR Hyperfine Co - PowerPoint PPT Presentation

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Disorder and Doubleexchange Spin Dynamics in La0'7Sr0'3MnO3 and La0'7Sr0'3CoO3 from NMR Hyperfine Co

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M.J.R. Hoch1, P.L. Kuhns1, W.G. Moulton1, A.P. Reyes1, M.A. Torija2, J.F. ... is attributed to the stronger double-exchange interaction in LSMO than in ... – PowerPoint PPT presentation

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Title: Disorder and Doubleexchange Spin Dynamics in La0'7Sr0'3MnO3 and La0'7Sr0'3CoO3 from NMR Hyperfine Co


1
Disorder and Double-exchange Spin Dynamics in
La0.7Sr0.3MnO3 and La0.7Sr0.3CoO3 from NMR
Hyperfine CouplingsM.J.R. Hoch1, P.L. Kuhns1,
W.G. Moulton1, A.P. Reyes1, M.A. Torija2, J.F.
Mitchell3 and C. Leighton2
Phys. Rev. B 75, 104421 (2007)
  • The magnetic oxides La1-x Srx MnO3 (LSMO) and
    La1-x Srx CoO3 (LSCO) have interesting and
    unusual properties, including very large
    magnetoresistance, that pose challenges to our
    understanding and opportunities for application
    in technology.


  • Changing Mn (LSMO) to Co (LSCO) results in
    striking changes in behavior and the present work
    has investigated samples of the two materials in
    their ferromagnetic-metallic phases (x0.3) in an
    effort to deepen our understanding of the
    competing interactions that determine the
    properties.
  • Using pulsed NMR information on the electron spin
    system has been obtained that shows that at low
    temperatures lattice disorder effects linked to
    Jahn-Teller distortion of the octahedral
    environment of the transition ions are more
    important in LSCO than in LSMO. This difference
    is attributed to the stronger double-exchange
    interaction in LSMO than in LSCO. Above 120 K,
    well below the Curie temperature of 360 K,
    lattice distortions are shown to kick in in
    LSMO. These effects can lead to localization of
    the electrons and the formation of spin polarons.
  • The three plots compare the results obtained for
    the two systems and show strikingly different
    behavior that is analyzed to obtain information
    on the roles of the underlying interactions.

Figure 1. Log-log plot og spin-lattice
relaxation rates versus ?Tfor x0.3 LMSO and
LSCO. The insert shows the importance of spin
waves on LSMO below 100 K.
(a)
(b)
Figure 2. Linewidths and relaxation rates Versus
T for (a) x0.3 LSMO, and (b) x0.3 LSCO.
1 National High Magnetic Field Laboratory, FSU,
Tallahassee, FL 2 Dept of Chemical Engineering
and Materials Science, University of Minnesota,
MN 3 Materials Science Division, Argonne National
Laboratory, Argonne, IL
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