2001
DOI: 10.1063/1.1379597
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Surface spin-glass behavior in La2/3Sr1/3MnO3 nanoparticles

Abstract: The low-temperature magnetic and transport properties of La2/3Sr1/3MnO3 nanoparticles have been investigated. It is found that a surface spin-glass behavior exists in La2/3Sr1/3MnO3 nanoparticles, which undergo a magnetic transition to a frozen state below 45 K. The low-temperature surface spin-glass behavior exists even at the highest field used (H=50 kOe). Moreover, the spin-glass-like transition disappears for particles above 50 nm. In addition, the suppressed low-field magnetoconductivity (LFMC) observed a… Show more

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Cited by 142 publications
(112 citation statements)
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“…More critical observation of the low-temperature Mössbauer data ͑12 and 4 K͒ revealed some very weak signal of sextet hyperfine splitting. Due to the low magnetic moment value for the sample and very small natural abundance of 57 Fe, the intensity of the observed signal is very weak. However, a more detailed fitting of the experimental data for 12 K in Fig.…”
Section: Mössbauer Spectroscopymentioning
confidence: 99%
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“…More critical observation of the low-temperature Mössbauer data ͑12 and 4 K͒ revealed some very weak signal of sextet hyperfine splitting. Due to the low magnetic moment value for the sample and very small natural abundance of 57 Fe, the intensity of the observed signal is very weak. However, a more detailed fitting of the experimental data for 12 K in Fig.…”
Section: Mössbauer Spectroscopymentioning
confidence: 99%
“…In addition to this, the technique is used to extract information about the oxidation state of the dopant cation involved in the spin coupling. 44,[57][58][59] Figures 8͑a͒ and 8͑b͒ show the EPR spectra of Zn 0.9 Fe 0.1 O recorded at room temperature and at 100 K. Both of the EPR spectra of Zn 0.9 Fe 0.1 O can be considered as a superposition of two overlapping signals, an intense and broad Gaussian signal ͑⌬H pp = 1675 G͒ with effective g factor g eff = 2.126 and another weak and narrow Lorentzian signal with g eff = 2.005. For the sake of convenience, the broad and narrow signals are designated as signal A ͑g eff = 2.126͒ and signal B ͑g eff = 2.005͒, respectively.…”
Section: Epr Measurementsmentioning
confidence: 99%
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“…These features make manganites the ideal system in which to study edge state physics among complex oxides systems. Although surface [11][12][13] and grain boundary effects [14][15][16][17] have been observed in manganites systems, it is very interesting to verify whether broken symmetry effect can introduce intrinsic edge states in manganites, especially when EPS dominates the system. For this reason, we have chosen a model system of La 0.325 Pr 0.3 Ca 0.375 MnO 3 (LPCMO) which has been well known for its striking large length scale EPS between ferromagnetic metallic (FM) and CE-type antiferromagnetic charge-ordered insulating (CE) phases 18 .…”
mentioning
confidence: 99%
“…There is also no irreversibility between ZFC and FC measurements, and this is in the more general terms thought due to the existence of short range ordering. 45 This ordering contributes differently to the total magnetization under ZFC and FC, thus provides nonoverlapping curves. The intraparticle interaction is also witnessed in the slight asymmetric loop shift of M-H curve under ZFC condition at 5 K (471 Oe, -563 Oe, inset, Fig.…”
Section: Resultsmentioning
confidence: 99%