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• W1964152068 abstract "Metallic surface states on semiconducting substrates provide an opportunity to study low-dimensional electrons decoupled from the bulk. Angle resolved photoemission is used to determine the Fermi surface, group velocity, and effective mass for surface states on $mathrm{Si}(111)sqrt{3}ifmmodetimeselsetexttimesfi{}sqrt{3}ensuremath{-}mathrm{Ag},$ $mathrm{Si}(111)sqrt{3}ifmmodetimeselsetexttimesfi{}sqrt{3}ensuremath{-}mathrm{Au},$ and $mathrm{Si}(111)sqrt{21}ifmmodetimeselsetexttimesfi{}sqrt{21}ensuremath{-}(mathrm{Ag}+mathrm{Au}).$ For $mathrm{Si}(111)sqrt{3}ifmmodetimeselsetexttimesfi{}sqrt{3}ensuremath{-}mathrm{Ag}$ the Fermi surface consists of small electron pockets populated by electrons from a few % excess Ag. For $mathrm{Si}(111)sqrt{21}ifmmodetimeselsetexttimesfi{}sqrt{21}ensuremath{-}(mathrm{Ag}+mathrm{Au})$ the pockets increase their size corresponding to a filling by three electrons per unit cell. The $sqrt{21}ifmmodetimeselsetexttimesfi{}sqrt{21}$ superlattice leads to an intricate surface umklapp pattern and to minigaps of 110 meV, giving an interaction potential of 55 meV for the $sqrt{21}ifmmodetimeselsetexttimesfi{}sqrt{21}$ superlattice." @default.
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• W1964152068 date "2002-11-01" @default.
• W1964152068 modified "2023-09-27" @default.
• W1964152068 title "Fermi surfaces of surface states on Si(111)-Ag, Au" @default.
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• W1964152068 doi "https://doi.org/10.1103/physrevb.66.205302" @default.
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