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Volumn 78, Issue 1, 2008, Pages

Time-resolved optical studies of spin and quasiparticle dynamics in colossal magnetoresistance materials: La0.67 Ca0.33 MnO3, La0.67 Sr0.33 MnO3, and Sr2 FeMoO6

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Indexed keywords


EID: 47349122266     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.78.014408     Document Type: Article
Times cited : (33)

References (35)
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    • We estimate the ∼1 μs relaxation time according to the relative magnitude of the negative transient reflectivity signal before the zero time-delay and at 1 ns position.
    • We estimate the ∼1 μs relaxation time according to the relative magnitude of the negative transient reflectivity signal before the zero time-delay and at 1 ns position.
  • 29
    • 47349130806 scopus 로고    scopus 로고
    • Since the magnitude of the transient reflectivity signal changes dramatically with applied external magnetic field and from sample to sample, we normalized the negative signal according to the peak value (when the negative signal reaches its maximum) for comparison. The normalization does not change the physical effect of the negative component.
    • Since the magnitude of the transient reflectivity signal changes dramatically with applied external magnetic field and from sample to sample, we normalized the negative signal according to the peak value (when the negative signal reaches its maximum) for comparison. The normalization does not change the physical effect of the negative component.
  • 34
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    • The solid curves in Fig. 2 are the combination of two power laws, which have been discussed in detail in the model part of the manuscript. The first one is the power law for T≤0.85 TC. This is mainly due to opening of the pseudogap; which is positive. The second one is the power law for 0.85 TC ≤T< TC; this is due to the loss of magnetization in the sample; which is negative.
    • The solid curves in Fig. 2 are the combination of two power laws, which have been discussed in detail in the model part of the manuscript. The first one is the power law for T≤0.85 TC. This is mainly due to opening of the pseudogap; which is positive. The second one is the power law for 0.85 TC ≤T< TC; this is due to the loss of magnetization in the sample; which is negative.
  • 35
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    • For a review, see, edited by Y. Tokura (Gordon and Breach, New York
    • For a review, see, Colossal Magnetoresistive Oxides, edited by, Y. Tokura, (Gordon and Breach, New York, 2000).
    • (2000) Colossal Magnetoresistive Oxides


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.