메뉴 건너뛰기




Volumn 64, Issue 19, 2001, Pages

Fermi surfaces of the two-dimensional surface states on vicinal Cu(111)

Author keywords

[No Author keywords available]

Indexed keywords

COPPER;

EID: 0035891388     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.64.195411     Document Type: Article
Times cited : (68)

References (40)
  • 24
    • 85038915597 scopus 로고    scopus 로고
    • Hoesch, diploma thesis
    • M. Hoesch, diploma thesis, University of Zurich, 1998.
    • (1998) University of Zurich
  • 33
    • 85038956947 scopus 로고    scopus 로고
    • A similar equation was derived by Beckmann, (Ref. to describe the line shape of a Tamm state on vicinal Cu(100). There, however, the integration was carried out over the width distribution of single terraces, rather than the average terrace length in the region probed by the surface state
    • A similar equation was derived by Beckmann et al. (Ref. 32) to describe the line shape of a Tamm state on vicinal Cu(100). There, however, the integration was carried out over the width distribution of single terraces, rather than the average terrace length in the region probed by the surface state.
  • 34
    • 85038898116 scopus 로고    scopus 로고
    • Our value of (formula presented) is obtained by fitting a Lorentzian convolved with a Gaussian of 31 meV FWHM to the low-energy side of the spectrum. The total linewidth amounts to 68 meV. Very recent measurements at the highest resolution interpolate to a room-temperature linewidth of (formula presented): G. Nicolay and F. Reinert (private communication)
    • Our value of (formula presented) is obtained by fitting a Lorentzian convolved with a Gaussian of 31 meV FWHM to the low-energy side of the spectrum. The total linewidth amounts to 68 meV. Very recent measurements at the highest resolution interpolate to a room-temperature linewidth of (formula presented): G. Nicolay and F. Reinert (private communication).
  • 40
    • 85038913739 scopus 로고    scopus 로고
    • In a Kronig-Penney model the shift of the band bottom is given by (formula presented) where (formula presented) is the integral over the potential barrier. To adjust the energy of the band bottom we used a potential of the form (formula presented) with (formula presented) and (formula presented)
    • In a Kronig-Penney model the shift of the band bottom is given by (formula presented) where (formula presented) is the integral over the potential barrier. To adjust the energy of the band bottom we used a potential of the form (formula presented) with (formula presented) and (formula presented).


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.