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Volumn 79, Issue 7, 2009, Pages

Local probing of charge and orbital-ordering-induced anisotropy with polarization-modulated infrared reflection difference microspectroscopy

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Indexed keywords


EID: 61949182266     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.79.073102     Document Type: Article
Times cited : (3)

References (18)
  • 7
    • 1342344138 scopus 로고    scopus 로고
    • 10.1103/PhysRevB.69.014407
    • K. Tobe, T. Kimura, and Y. Tokura, Phys. Rev. B 69, 014407 (2004). 10.1103/PhysRevB.69.014407
    • (2004) Phys. Rev. B , vol.69 , pp. 014407
    • Tobe, K.1    Kimura, T.2    Tokura, Y.3
  • 14
    • 0018444443 scopus 로고
    • 10.1366/0003702794926038
    • L. A. Nafie and M. Diem, Appl. Spectrosc. 33, 130 (1979). 10.1366/0003702794926038
    • (1979) Appl. Spectrosc. , vol.33 , pp. 130
    • Nafie, L.A.1    Diem, M.2
  • 15
    • 61949389479 scopus 로고    scopus 로고
    • The average base line of the PM-RD values is not at the zero level but is found to have a negative value. This comes from, for example, polarization artifacts of the PEM and the optical setup. The amplitude of the PM-RD signal, however, is hardly affected by such artifacts (Ref. and
    • The average base line of the PM-RD values is not at the zero level but is found to have a negative value. This comes from, for example, polarization artifacts of the PEM and the optical setup. The amplitude of the PM-RD signal, however, is hardly affected by such artifacts (Ref. and M. Schmidt, to be published), hence it is a suitable indicator of the sample anisotropy irrespective of the experimental artifacts.
    • Schmidt, M.1
  • 16
    • 33644546389 scopus 로고    scopus 로고
    • 10.1088/0034-4885/69/3/R06
    • Y. Tokura, Rep. Prog. Phys. 69, 797 (2006). 10.1088/0034-4885/69/3/R06
    • (2006) Rep. Prog. Phys. , vol.69 , pp. 797
    • Tokura, Y.1
  • 17
    • 61949351503 scopus 로고    scopus 로고
    • The angle-dependent PM-RD values can be fitted by a well-defined formula, as shown in Ref., where the parameters used for the fitting were found to be consistent with the reflectivities shown in Figs. 1 1, with the reflectivity difference of, e.g., ∼10% at 8°C for the domain A.
    • The angle-dependent PM-RD values can be fitted by a well-defined formula, as shown in Ref., where the parameters used for the fitting were found to be consistent with the reflectivities shown in Figs. 1 1, with the reflectivity difference of, e.g., ∼10% at 8°C for the domain A.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.