2011
DOI: 10.1016/j.physleta.2011.02.026
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Analysis of colossal magnetoresistance effect in perovskite oxide heterostructures

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Cited by 2 publications
(2 citation statements)
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“…where R 0 is the resistance at zero field and R H is the resistance at field H. Interestingly, the MR value in LSMO/Si-NTs exhibits a crossover behavior with decreasing the temperature, from negative MR (NMR) at RT to PMR at ∼150 K (under 1 According to literature, 10,11,24 the electron filling in the energy band of t 2g…”
Section: Resultsmentioning
confidence: 98%
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“…where R 0 is the resistance at zero field and R H is the resistance at field H. Interestingly, the MR value in LSMO/Si-NTs exhibits a crossover behavior with decreasing the temperature, from negative MR (NMR) at RT to PMR at ∼150 K (under 1 According to literature, 10,11,24 the electron filling in the energy band of t 2g…”
Section: Resultsmentioning
confidence: 98%
“…According to literature, ,, the electron filling in the energy band of t 2g ↓ could be the origin of the PMR, where the electrons in t 2g ↓ act as minority spin carriers (MISCs) that have opposite spin direction to the majority spin carriers. In such case, the occupation of electrons in t 2g ↓ could lead to spin-flipping scattering and contribute to the device resistance.…”
Section: Resultsmentioning
confidence: 99%