1998
DOI: 10.1016/s0168-583x(98)00385-1
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The broadening of energy spectra of atoms scattered by a solid surface under molecular ion bombardment

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Cited by 7 publications
(4 citation statements)
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“…Equation ͑3.1͒ does not consider any inelastic effects such as energy loss and straggling. These effects give rise to an asymmetric shape of the spectra, which is discussed in more detail by Wojciechowski et al 7 Närmann et al [23][24][25] These authors use analytic functions to describe the energetic distributions of the forward scattered beam; we found the best agreement with our experimental results when fitting a universal so-called exponentially modified Gauss function ͑EMG͒:…”
Section: Figure 4͑a͒supporting
confidence: 76%
See 1 more Smart Citation
“…Equation ͑3.1͒ does not consider any inelastic effects such as energy loss and straggling. These effects give rise to an asymmetric shape of the spectra, which is discussed in more detail by Wojciechowski et al 7 Närmann et al [23][24][25] These authors use analytic functions to describe the energetic distributions of the forward scattered beam; we found the best agreement with our experimental results when fitting a universal so-called exponentially modified Gauss function ͑EMG͒:…”
Section: Figure 4͑a͒supporting
confidence: 76%
“…4 In our prior work on H 2 ϩ and N 2 ϩ scattered off the ͑110͒and ͑111͒-faces of palladium under grazing incidence, we could show that parallel to a low-index direction, mainly rotational excitation occurs whereas for high-index scattering, vibrational excitation is the main reason for dissociation. [5][6][7] In contrast to molecules such as H 2 or O 2 , charge transfer processes during the interaction of N 2 with metal surfaces are of minor importance for the dissociation process, [8][9][10] even though to a small extent electronical excitation due to violent collisions with surface atoms is possible. 11 N 2 is therefore a perfect system for a direct comparison of N 2 ϩ scattering experiments with purely classical simulations for neutral N 2 .…”
Section: Introductionmentioning
confidence: 99%
“…However it is still physically unclear how the screening phenomenon effectively occurs for the excited states of atomic structures where one has noted that a simplified and systematic analytical model is almost entirely absent. Analytical methods for screened atoms are important for studying electronic properties in metalinsulator transitions, charge transport in materials, impurities in semiconductors [30][31][32], charged polymer gels [33][34][35], properties of nanostructures [36,37], molecules adsorbed in metals [38][39][40][41][42][43], hydrogen under pressure, as well as other interesting applications [44][45][46][47][48][49].…”
Section: Introductionmentioning
confidence: 99%
“…The remaining broad part of the spectrum has a pronounced asymmetry. The low-energy tail is well described in terms of energy loss and energy loss straggling for the atoms penetrating deeper into the bulk and traveling longer inside the solid . The focus of our study is the high-energy tail.…”
Section: Introductionmentioning
confidence: 99%