1987
DOI: 10.1103/physrevb.35.975
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Effective mass of image-potential states

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Cited by 138 publications
(59 citation statements)
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“…We synthesized two compounds (scheme 1: 2 and 5) having redox-active terminal groups with lowest unoccupied molecular orbitals (LUMOs) having energies close to, but greater than, the Fermi levels of the electrodes (EGaIn ≈ -4.3 eV, Ag ≈ -4.5 eV). 43,44,45 The synthesis of these compounds is described in the Supporting Information. We do not know the exact energies of the LUMOs of these compounds, but we do know that the LUMO of 2 is higher in energy than the LUMO of 5, because the addition of a second aromatic ring increases the electron affinity of the moiety.…”
Section: Resultsmentioning
confidence: 99%
“…We synthesized two compounds (scheme 1: 2 and 5) having redox-active terminal groups with lowest unoccupied molecular orbitals (LUMOs) having energies close to, but greater than, the Fermi levels of the electrodes (EGaIn ≈ -4.3 eV, Ag ≈ -4.5 eV). 43,44,45 The synthesis of these compounds is described in the Supporting Information. We do not know the exact energies of the LUMOs of these compounds, but we do know that the LUMO of 2 is higher in energy than the LUMO of 5, because the addition of a second aromatic ring increases the electron affinity of the moiety.…”
Section: Resultsmentioning
confidence: 99%
“…Energy relative to vacuum level, eV The difference in upper band edge energies also affects the effective mass calculated by the means of Giesen, et al 50 In their calculation, the work function was taken as 4.56 eV, and the various parameters necessary in the calculation are listed below: 143 In Figure They may also be expected to scatter outgoing photoelectrons, altering both the direction and kinetic energy of the photoelectrons.…”
Section: Fiqure 27mentioning
confidence: 99%
“…65 ,40 When image potential states were observed, the threshold for unacceptably strong space charge broadening was reported to occur at about 5xl0 4 The angular resolution in this experiment was ±2. 50 ---------1.,. showing the electrostatic potentials is given in Figure 18.…”
mentioning
confidence: 99%
“…The electron motion parallel to the surface is quasifree with effective mass close to one. 48,51 The higher is n, the further from the surface is located the excited electron, and the smaller is its coupling with metal bulk electrons so that the lifetime of the image states increases as n 3 . 12,29,[50][51][52][53][54] The hybridization between QWSs and ISs would alter the weight of the QWS wave function inside the metal film, shifting part of the electron density into the vacuum.…”
Section: Introductionmentioning
confidence: 99%
“…The ISs correspond to an excited electron bound in front of the metal surface by the image charge potential. When electron penetration into the metal is prohibited by the projected band gap, ISs form a Rydberg series converging toward the vacuum level E V with energies at¯ given by 12,13,[48][49][50][51] …”
Section: Introductionmentioning
confidence: 99%