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Oxygen atoms and molecules at Lanthanum-Strontium Manganite surfaces

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 Added by Walter Harrison
 Publication date 2009
  fields Physics
and research's language is English




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A localized description, rather than energy bands, is appropriate for the manganite substrate. Empty substrate levels lower in energy than occupied oxygen levels indicate need for further terms beyond the Local Density Approximation. So also does van-der-Waals interaction between the two. Methods to include both are suggested by related, exactly soluble, two-electron problems. The descriptions of the electronic structure of the molecule and a LaSrMnO3 (LSM) substrate are greatly simplified to allow incorporation of these effects and to treat a range of problems involving the interactions between oxygen atoms, or oxygen molecules, and such a substrate. These include elastic impacts, impacts with electronic transitions, and impacts with phonon excitation. They provide for capture of the atoms or molecules by the surface, leaving the neutral molecule strongly bound over a Mn(4+) site. It is found that oxygen vacancies in LSM diffuse as a neutral species, and can appear at the surface. Bound molecules tend to avoid sites next to vacancies but, if there, should drop one atom into the vacancy leaving the remaining triplet oxygen atom bound to the resulting ideal surface, with no need for spin flips nor successive ionization steps.



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We report on the magnetic, resistive, and structural studies of perovskite La$_{1/3}$Sr$_{2/3}$CoO$_{3-delta}$. By using the relation of synthesis temperature and oxygen partial pressure to oxygen stoichiometry obtained from thermogravimetric analysis, we have synthesized a series of samples with precisely controlled $delta=0.00-0.49$. These samples show three structural phases at $delta=0.00-0.15$, $approx0.25$, $approx0.5$, and two-phase behavior for other oxygen contents. The stoichiometric material with $delta=0.00$ is a cubic ferromagnetic metal with the Curie temperature $T_{rm C}=274$ K. The increase of $delta$ to 0.15 is followed by a linear decrease of $T_{rm C}$ to $approx$ 160 K and a metal-insulator transition near the boundary of the cubic structure range. Further increase of $delta$ results in formation of a tetragonal $2a_ptimes 2a_p times 4a_p$ phase for $deltaapprox 0.25$ and a brownmillerite phase for $deltaapprox0.5$. At low temperatures, these are weak ferromagnetic insulators (canted antiferromagnets) with magnetic transitions at $T_{rm m}approx230$ and 120 K, respectively. At higher temperatures, the $2a_ptimes 2a_p times 4a_p$ phase is $G$-type antiferromagnetic between 230 K and $approx$360 K. Low temperature magnetic properties of this system for $delta<1/3$ can be described in terms of a mixture of Co$^{3+}$ ions in the low-spin state and Co$^{4+}$ ions in the intermediate-spin state and a possible spin transition of Co$^{3+}$ to the intermediate-spin state above $T_{rm C}$. For $delta>1/3$, there appears to be a combination of Co$^{2+}$ and Co$^{3+}$ ions, both in the high-spin state with dominating antiferromagnetic interactions.
132 - Walter A. Harrison 2008
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