2000
DOI: 10.1103/physrevb.61.11373
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Effect of annealing temperature on local distortion ofLa0.67Ca0.33MnO<

Abstract: Mn K-edge fluorescence data are presented for thin film samples (3000Å) of Colossal Magnetoresistive (CMR) La 0.67 Ca 0.33 MnO 3 : as-deposited, and post-annealed at 1000 K and 1200 K. The local distortion is analyzed in terms of three contributions: static, phonon, and an extra, temperature-dependent, polaron term. The polaron distortion is very small for the as-deposited sample and increases with the annealing temperature. In contrast, the static distortion in the samples decreases with the annealing tempera… Show more

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Cited by 30 publications
(17 citation statements)
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“…28͒ with the quantity S 0 2 N fixed at 4.3, based on earlier work. 17,18,20 In these fits, only and r were varied. The value of 2 for the Mn-O peak was obtained for each temperature and magnetic field.…”
Section: Xafs Data Analysismentioning
confidence: 99%
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“…28͒ with the quantity S 0 2 N fixed at 4.3, based on earlier work. 17,18,20 In these fits, only and r were varied. The value of 2 for the Mn-O peak was obtained for each temperature and magnetic field.…”
Section: Xafs Data Analysismentioning
confidence: 99%
“…Here T 2 is a measure of the phonon contribution ͑the DebyeWaller contribution͒, FP 2 is the full polaronlike distortion obtained at high temperature, which is defined as the difference between data 2 and T 2 at high temperatures ͑above T c ), and data 2 is extracted from fits of the XAFS data, 18,20 for the Mn-O peak. ⌬ 2 is zero above T c and ln(⌬ 2 ) increases linearly as the sample's magnetization increases.…”
Section: Of 2 Vs Tmentioning
confidence: 99%
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“…When polarons form there is a large additional increase in the local distortions about a lattice site, generally referred to as a Jahn-Teller (JT) distortion [3,8,9,10,11,12]. This distortion enhances the increase in resistivity as the sample becomes paramagnetic [13,14,15].…”
Section: Polaron Systemsmentioning
confidence: 99%
“…The ferromagnetism of LSMO can be tuned by varying the doping concentration and oxygen content [9][10][11]. By varying the deposition temperature and oxygen partial pressure, the oxygen content in LSMO thin films can be controlled [12][13][14]. Also the oxygen partial pressure during deposition plays a very crucial role in shaping the microstructure and surface morphology and hence the interface quality of the thin film [15].…”
Section: Introductionmentioning
confidence: 99%