2011
DOI: 10.1021/jp205902k
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The Effects of Electron–Hole Pair Coupling on the Infrared Laser-Controlled Vibrational Excitation of NO on Au(111)

Abstract: In this work, we present theoretical simulations of laser-driven vibrational control of NO adsorbed on a gold surface. Our goal is to tailor laser pulses to selectively excite specific modes and vibrational eigenstates, as well as to favor photodesorption of the adsorbed molecule. To this end, various control schemes and algorithms are applied. For adsorbates at metallic surfaces, the creation of electron-hole pairs in the substrate is known to play a dominant role in the transfer of energy from the system to … Show more

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Cited by 11 publications
(3 citation statements)
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References 68 publications
(90 reference statements)
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“…TDDVR 6D QD outcomes 42 In the realm of surface science, elhp excitations impart substantial effects on the dissociative chemisorption, inelastic scattering, and external field induced (vibrational excitation, relaxation, dissipation, and non-adiabatic electron transfer) phenomena. 46,[108][109][110][111][112][113][114][115] In this context, various theoretical approaches, namely, electronic friction (EF) 88 [local density friction approximation (LDFA) 46 and orbital dependent friction (ODF) 46,116,117 ], independent electron surface hopping (IESH), 112,118 reduced density matrix, [119][120][121] EH (phonon + elhp), 105,106 and stochastic wave packet approach, 122 have been developed during the past few decades. Those theoretical treatments unveiled the crucial contribution of elhp excitations on the state-to-state vibrational transition probabilities at higher surface temperature situations.…”
Section: Introductionmentioning
confidence: 99%
“…TDDVR 6D QD outcomes 42 In the realm of surface science, elhp excitations impart substantial effects on the dissociative chemisorption, inelastic scattering, and external field induced (vibrational excitation, relaxation, dissipation, and non-adiabatic electron transfer) phenomena. 46,[108][109][110][111][112][113][114][115] In this context, various theoretical approaches, namely, electronic friction (EF) 88 [local density friction approximation (LDFA) 46 and orbital dependent friction (ODF) 46,116,117 ], independent electron surface hopping (IESH), 112,118 reduced density matrix, [119][120][121] EH (phonon + elhp), 105,106 and stochastic wave packet approach, 122 have been developed during the past few decades. Those theoretical treatments unveiled the crucial contribution of elhp excitations on the state-to-state vibrational transition probabilities at higher surface temperature situations.…”
Section: Introductionmentioning
confidence: 99%
“…These constraints are not met for most molecule-surface systems, where multiple minima are connected by low-energy barriers along large amplitude diffusion coordinates. Only recently were these limitations addressed adequately, [38][39][40] where the adsorbate was embedded in an electron gas of variable density to mimic the position-dependence of the non-adiabatic coupling. In the model, numerical integration of the gradient operator was used to ensure proper treatment of anharmonicity.…”
Section: Introductionmentioning
confidence: 99%
“…It is the main goal of the present work to develop a physically sound model that goes beyond these limitations while keeping its most attractive features. Since the position-dependent anharmonic rate model introduced recently [38][39][40] cannot be extended straightforwardly to treat STM-induced excitations, an alternative derivation is proposed. To avoid the pitfalls associated with the identification and the characterization of a single adsorbate resonance, the model of Gao et al [49][50][51][52] is reinterpreted using source-bridgesink terminology, where the source and sink density of states are projected on a physical bridge state located at the position of the adsorbate, hence allowing to recover the positiondependence of the non-adiabatic couplings.…”
Section: Introductionmentioning
confidence: 99%