CMR manganites are important to spintronics for two reasons. First,
they exhibit an extremely large drop in electrical resistance (the
CMR effect) when a magnetic field is applied. Second, for some cases,
CMR materials conduct electricity via electrons of only one spin
(half-metallic ferromagnetism). However, a complete understanding
of the charge and spin state of the manganese atoms, crucial to
determining and engineering the properties of these materials, is
still lacking.
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| The Mn 3d levels are split into two subsets: t2g
(threefold degenerate) and eg (twofold degenerate). The t2g
electrons, lower in energy, are more localized; the outermost eg
electrons are more delocalized, capable of hopping from site to
site provided that the t2g spins on adjacent manganese
atoms are parallel. According to the Jahn-Teller effect, as soon
as an electron hops into an empty eg orbital, a distortion of the
octahedral cage of O atoms lowers the symmetry and further splits
the eg and t2g levels. The electron is now more tightly
bound, forming a so-called lattice polaron. |
To explain the magnetoconductive properties of these manganites,
in which the manganese is present in at least two different valence
states (Mn3+ and Mn4+), Zener proposed the mechanism of double exchange
(DE). According to DE, the alignment of adjacent localized t2g spins
on manganese atoms rules the dynamics of itinerant eg carriers,
which hop from one atom to the next to yield electrical conductivity.
If adjacent t2g spins are parallel (the ferromagnetic state), conduction
is favored; if they are randomly aligned (the paramagnetic high-temperature
state), conductivity drops dramatically.
While Zener's DE model provides a qualitatively correct picture
of the CMR effect, theoretical calculations have shown that DE alone
is insufficient to account for the observed CMR resistance. An additional
consideration is the localization of itinerant eg electrons by Jahn-Teller
distortions of the octahedral cage of oxygen atoms surrounding each
manganese atom.
A Jahn-Teller distortion can take place when an electron hops
into an empty eg orbital so that, while hopping from site to site,
the electron "drags" the lattice distortions after itself. The electron
with its accompanying lattice distortion forms a so-called "lattice
polaron." Since the surrounding oxygen atoms are much more massive
than the bare electron, the polaron behaves as a negatively charged
particle with a larger mass and lower mobility than an isolated
electron.
In this study, the temperature-dependent evolution of the electronic
and crystal structure of a prototypical CMR compound, La0.7Sr0.3MnO3
(LSMO), was investigated. Spectroscopic experiments were performed
using the multitechnique spectrometer/diffractometer at ALS Beamline
4.0.2. As the LSMO compound was heated through its Curie temperature
(TC), core photoelectron spectroscopy data provided direct evidence
for charge localization onto the manganese atom via a change in
the manganese 3s multiplet splitting and for chemical shifts in
the core levels of the other atoms in the sample. Valence photoemission
spectra also showed parallel changes with temperature. Additional
hard-x-ray EXAFS measurements detected the presence of Jahn-Teller
lattice distortions in the oxygen octahedra surrounding manganese
atoms as the temperature rose above TC.
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Mn 3s and O 1s photoelectron spectra. (a)
The Mn 3s spectrum exhibits a doublet due to multiplet splitting.
The energy separation of this doublet depends on the net
spin of the Mn atom, providing a direct and element-specific
measure of its magnetic moment. The Mn 3s splitting changes
markedly as the temperature increases from TC to a saturation
temperature TMAX, indicating an increase in the magnetic
moment corresponding to the transfer of about one electron
to Mn. (b) The "bulk" O 1s binding energy shows
a concomitant increase, consistent with charge transfer
to Mn. Similar shifts are also found for La and Sr.
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These experiments permitted the detection of polaron formation
via its effects on the manganese and other atoms in the LSMO.
This challenges the long-standing belief that LSMO is a simple
DE system that can be described without the formation of polarons.
Therefore, the presence of polarons above TC is a general
defining characteristic of all CMR materials, bringing unity to
their theoretical description. Beyond spintronic applications,
these results could also have implications for the magnetic states
of atoms under high pressure, as in the Earth's core.
Research conducted by N. Mannella, B.S. Mun, and C.S. Fadley (University
of California, Davis, and Berkeley Lab); A. Rosenhahn, C.H. Booth,
S. Marchesini, and S.-H. Yang (Berkeley Lab); K. Ibrahim (Beijing
Synchrotron Radiation Laboratory, China, and Berkeley Lab); and
Y. Tomioka (Correlated Electron Research Center, Japan).
Research funding: U.S. Department of Energy, Office of Basic
Energy Sciences (BES), Materials Sciences and Engineering Division.
Operation of the ALS is supported by BES.
Publication about this research: N. Mannella, A. Rosenhahn, C.H.
Booth, S. Marchesini, B.S. Mun, S.-H. Yang, K. Ibrahim, Y. Tomioka,
and C.S. Fadley, "Direct Observation of High-Temperature Polaronic
Behavior in Colossal Magnetoresistive Manganites," Phys.
Rev. Lett. 92, 166401 (2004).
ALSNews
Vol. 249, January 26, 2005
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