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Volumn 81, Issue 12, 2010, Pages

Multichannel multiple scattering calculation of L2,3 -edge spectra of TiO2 and SrTiO3: Importance of multiplet coupling and band structure

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EID: 77955166955     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.81.125121     Document Type: Article
Times cited : (142)

References (19)
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    • P. Krüger and C. R. Natoli, Phys. Rev. B 70, 245120 (2004). 10.1103/PhysRevB.70.245120
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    • Krüger, P.1    Natoli, C.R.2
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    • G. van der Laan, Phys. Rev. B 41, 12366 (1990). 10.1103/PhysRevB.41.12366
    • (1990) Phys. Rev. B , vol.41 , pp. 12366
    • Van Der Laan, G.1
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    • 0000342836 scopus 로고
    • This is equivalent to the LDA+U method from the localized limit in absence of spin and orbital polarization, where Δ Ed = (5- nd ) (U-J ) /10 with nd being the ground-state d -electron number, see, e.g., 10.1103/PhysRevB.49.14211
    • This is equivalent to the LDA + U method from the localized limit in absence of spin and orbital polarization, where Δ E d = (5 - n d) (U - J) / 10 with n d being the ground-state d -electron number, see, e.g., M. T. Czyzyk and G. A. Sawatzky, Phys. Rev. B 49, 14211 (1994). 10.1103/PhysRevB.49.14211
    • (1994) Phys. Rev. B , vol.49 , pp. 14211
    • Czyzyk, M.T.1    Sawatzky, G.A.2
  • 19
    • 77955160657 scopus 로고    scopus 로고
    • note
    • Open-boundary conditions in the multiple-scattering calculation correspond to an embedding of the cluster into a background of free electron states. For very small cluster sizes, the coupling to the free electron states leads to an extra broadening of the spectra (especially for the single atom "1" in Fig.) as well as to a "metallic" peak at the Fermi cutoff (marked with a dotted line in Fig.). However, these finite-size effects vanish quickly with increasing cluster size.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.