2017
DOI: 10.1088/2053-1591/aa8bc7
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Interaction of slow highly charged ions with a metal surface covered with a thin dielectric film. The role of the neutralization energy in the nanostructures formation

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Cited by 5 publications
(10 citation statements)
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“…For the metal surface parameters, within the Sommerfeld model, we use the value of the work function φ = 5eV and for the potential depth U 0 = 15eV. The dielectric film is characterized by the width s 0 , and by the dielectric constants = 2, 4 and 8.We analyze the arbitrary collision geometry for the angles of incidence Φ in = π/2, 3π/8 and π/4.Due to the interaction of the HCI with solid surface the ionic charge decreases in time according to the cascade neutralization scenario Q = Z → Z − 1 → .... → Q fin , see The neutralization process in the MDV-system we treat within the framework of the TVM and micro-staircase model (Majkić et al, 2017(Majkić et al, , 2019. According to the TVM the state of the active electron e − is described by two state vectors |Ψ 1 (t) and |Ψ 2 (t) , which simultaneously evolve in two opposite directions of time.…”
Section: Neutralization Dynamics Of the Hci In The Mdv-systemmentioning
confidence: 99%
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“…For the metal surface parameters, within the Sommerfeld model, we use the value of the work function φ = 5eV and for the potential depth U 0 = 15eV. The dielectric film is characterized by the width s 0 , and by the dielectric constants = 2, 4 and 8.We analyze the arbitrary collision geometry for the angles of incidence Φ in = π/2, 3π/8 and π/4.Due to the interaction of the HCI with solid surface the ionic charge decreases in time according to the cascade neutralization scenario Q = Z → Z − 1 → .... → Q fin , see The neutralization process in the MDV-system we treat within the framework of the TVM and micro-staircase model (Majkić et al, 2017(Majkić et al, , 2019. According to the TVM the state of the active electron e − is described by two state vectors |Ψ 1 (t) and |Ψ 2 (t) , which simultaneously evolve in two opposite directions of time.…”
Section: Neutralization Dynamics Of the Hci In The Mdv-systemmentioning
confidence: 99%
“…The states of the active electron at the time t (at ion-surface distance R) between the initial time t in and the final time t f in are expressed via intermediate eigenstates |µ M (R) and |ν A (R) of the in-HamiltonianĤ 1 (R) and the out-HamiltonianĤ 2 (R), respectively (Nedeljković et al, 2012;Nedeljković et al, 2016). By the ap-propriate expressions of the HamiltoniansĤ 1 (R) andĤ 2 (R) we take into account the polarization of the metal surface and the polarization of the ionic core, respectively, as well as the effect of the dielectric film (Majkić et al, 2017). The corresponding eigenenergies are E M = −γ 2 M /2 (γ M is the continous energy parameter) and…”
Section: Neutralization Dynamics Of the Hci In The Mdv-systemmentioning
confidence: 99%
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