2000
DOI: 10.1103/physrevb.61.8489
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Work-function anisotropy in noble metals: Contributions fromdstates and effects of the surface atomic structure

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Cited by 61 publications
(47 citation statements)
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“…41 for the clean Cu(111) and Pb(111) surfaces we estimate a work function of 4.85 and 3.86 eV, respectively, in excellent agreement with the reference values, that are in the range from 4.90 to 5.01 eV 42 for Cu(111), and 3.83 eV for Pb(111). 43 ∆W can be related to the dipole moment induced in the substrate by the presence of the RG adatom, ∆µ, using the Helmholtz equation:…”
supporting
confidence: 69%
“…41 for the clean Cu(111) and Pb(111) surfaces we estimate a work function of 4.85 and 3.86 eV, respectively, in excellent agreement with the reference values, that are in the range from 4.90 to 5.01 eV 42 for Cu(111), and 3.83 eV for Pb(111). 43 ∆W can be related to the dipole moment induced in the substrate by the presence of the RG adatom, ∆µ, using the Helmholtz equation:…”
supporting
confidence: 69%
“…Our calculated work-functions are smaller than the experimental values [37][38][39]. Our calculated values show a systematic decrease in the work-function for clean surfaces with decrease in coordination of substrate atoms.…”
Section: Iii3 Vibrational Properties and Work-functioncontrasting
confidence: 45%
“…We compute  for Au(111) to be 5.55 eV, in good agreement with experimental values and prior calculations. [44] Values of  for BDA-covered Au(111), as shown in Fig. 2b), are all smaller than that of bare Au(111), implying the total effective dipole moments of both BDA adsorbate phases, including both intrinsic and binding-induced contributions, point toward the Au surface [45].…”
mentioning
confidence: 99%