2012
DOI: 10.1103/physrevb.86.125444
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Lifetime reduction of surface states at Cu, Ag, and Au(111) caused by impurity scattering

Abstract: We present density-functional results on the lifetime of the (111) surface state of the noble metals. We consider scattering on the Fermi surface caused by impurity atoms belonging to the 3d and 4sp series. The results are analyzed with respect to film thickness and with respect to separation of scattering into bulk or into surface states. While for impurities in the surface layer the overall trends are similar to the long-known bulk-state scattering, for adatom-induced scattering we find a surprising behavior… Show more

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Cited by 12 publications
(19 citation statements)
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References 46 publications
(68 reference statements)
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“…The importance of resonant scattering in metals is well known, including trivial surface states as e.g. the (111) surface states of the noble metals 25,27 . Here we have seen that the TSS are just as susceptible to resonant scattering, with the difference that the scattering is mostly forward-directed and exact or near backscattering is absent or strongly suppressed, respectively.…”
Section: Discussionmentioning
confidence: 99%
See 1 more Smart Citation
“…The importance of resonant scattering in metals is well known, including trivial surface states as e.g. the (111) surface states of the noble metals 25,27 . Here we have seen that the TSS are just as susceptible to resonant scattering, with the difference that the scattering is mostly forward-directed and exact or near backscattering is absent or strongly suppressed, respectively.…”
Section: Discussionmentioning
confidence: 99%
“…The perturbed potential and density were also calculated within the LDA. The T -matrix and scattering rates were calculated in the KKR representation as described elsewhere 24,25 . Structural relaxations around the vacancy can be important in the calculation of the vacancy-formation energy.…”
Section: Introductionmentioning
confidence: 99%
“…From the latter, the scattering probability and the momentum-as well as the spin-flip relaxation rate can be quantitatively determined via the spin-dependent scattering matrix. [20][21][22][23][24] Knowledge of the spin-dependent scattering probability allows us to employ the Boltzmann equation for spin Hall transport. 12,36,37 Then, the spin Hall conductivity as well as the spin Hall angle are calculated.…”
Section: Theorymentioning
confidence: 99%
“…[18][19][20][21][22][23][24][25] However, little is known about these effects in metallic thin films with thickness in the nanometer regime. Owing to the breaking of translational symmetry in thin films, many parameters have to be taken into account, such as the thickness and the crystalline orientation of the films.…”
Section: Introductionmentioning
confidence: 99%
“…The quasistationary surface state resonances or image potential resonances (IPRs) are then formed. The total decay rate =h/τ (τ being the lifetime) of an electronic excitation in the quasistationary IPR state is thus determined by four contributions: 26,31 inelastic electron-electron scattering 4,5 (decay rate ee ), electron-phonon interaction 32,33 ( ep ), electron-defect scattering 34 ( ed ), and energy-conserving resonant one-electron tunneling into the bulk [35][36][37][38] ( 1e ). The one-electron transfer into the substrate is thought to be faster than the many-body decay and so to dominate the population decay of the quasistationary states at low defect surfaces.…”
Section: Introductionmentioning
confidence: 99%