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Volumn 79, Issue 13, 2009, Pages

Absence of magnetic-field-induced effects in the mid-infrared transmission of La2-x Srx CuO4 thin films

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EID: 65149087209     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.79.134503     Document Type: Article
Times cited : (4)

References (50)
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    • Although the two might be strongly coupled.
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    • Film thickness must not be large as to render the sample nontransparent, but on the other hand it must be large enough to produce significant absorption of electromagnetic radiation. For example, for the film with x=0.10 the absolute value of transmission is reduced by about 50% compared with the bare substrate.
    • Film thickness must not be large as to render the sample nontransparent, but on the other hand it must be large enough to produce significant absorption of electromagnetic radiation. For example, for the film with x=0.10 the absolute value of transmission is reduced by about 50% compared with the bare substrate.
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    • The Néel temperatures for film are not available. The temperatures shown in the table are for bulk samples with similar doping levels: A. Gozar, B. S. Dennis, G. Blumberg, Seiki Komiya, and Yoichi Ando, Phys. Rev. Lett. 93, 027001 (2004). 10.1103/PhysRevLett.93.027001
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    • Previous IR measurements on LSAO did not detect any temperature dependence in this frequency range (Refs.).
    • Previous IR measurements on LSAO did not detect any temperature dependence in this frequency range (Refs.).
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    • The optical conductivity data for LSCO with similar doping level (Ref.) were fit with DL model, (ω) =1- ωD2 ω (ω+i/τ) + ωL2 ω02 - ω2 -iωγ, with ωD =6300 cm-1, τ=115 cm-1, ω0 =250 cm-1, ωL =13000 cm-1, and γ=4000 cm-1.
    • The optical conductivity data for LSCO with similar doping level (Ref.) were fit with DL model, (ω) =1- ωD2 ω (ω+i/τ) + ωL2 ω02 - ω2 -iωγ, with ωD =6300 cm-1, τ=115 cm-1, ω0 =250 cm-1, ωL =13000 cm-1, and γ=4000 cm-1.


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