Abstract:Ne atoms with energies of ≤3
keV are diffracted under grazing
angles of incidence from a LiF(001) surface. For a small momentum
component of the incident beam perpendicular to the surface, we observe
an increase in the elastic rainbow angle together with a broadening
of the inelastic scattering profile. We interpret these two effects
as the refraction of the atomic wave in the attractive part of the
surface potential. We use a fast, rigorous dynamical diffraction calculation
to find a projectile–surface potent… Show more
“…The time step also should be adapted to smaller values. Using the ASCA, only the slow motion in the (y,z) plane has to be considered and wave packet propagation 11,[31][32][33] or close coupling approaches 34,35 have been successfully applied. The accuracy of the axial channeling approximation was investigated in detail by extensive 3D calculations compared with the simplified 2D ASCA.…”
Section: Quantum Scattering Modelsmentioning
confidence: 99%
“…In ref. 35, diffraction data from neon displayed in Fig. 7 and 8 were compared with a recent ab initio calculation of the PEL by Miraglia and Gravielle 79 who kindly accepted to provide a compact description of their results in the form of effective binary interaction potentials.…”
Section: Quantitative Comparison With Quantum Theorymentioning
confidence: 99%
“…79 optimized to the data by a new close coupling code 106 providing the first quantitative agreement. 35 vibrational transition can be calculated exactly as p e = |hc|e idkz |ci| 2 which, for an atom initially in the vibrational ground state is proportional to p e p e ÀEr/h oD (eqn (3)). This probability is significant only when the recoil energy is less than a vibrational energy quantum 21 and can be identified as the Mössbauer-Lamb-Dicke probability for recoil-less photon emission characteristic of a trapped atom, for instance in an optical lattice.…”
Section: Quantum Binary Scatteringmentioning
confidence: 99%
“…Experimentally, a combined GIFAD and HAS study of a thin overlayer, for instance of graphene, 100 would probably help in the identification of specific vibration modes and allow significant progress. Regarding elastic diffraction, the recent progress 35 should allow for the implementation of a crystallographic software starting with a qualitative adjustment of surface atoms coordinates and effective binary interaction potentials by the HCW model and then final quantitative optimization by quantum scattering programs.…”
In the elastic regime, GIFAD is equivalent to TEAS with an effective energy E⊥ between 1 meV and 1 eV providing a high sensitivity to topology and to attractive forces. The inelastic regime merges to the classical limit and is still in development.
“…The time step also should be adapted to smaller values. Using the ASCA, only the slow motion in the (y,z) plane has to be considered and wave packet propagation 11,[31][32][33] or close coupling approaches 34,35 have been successfully applied. The accuracy of the axial channeling approximation was investigated in detail by extensive 3D calculations compared with the simplified 2D ASCA.…”
Section: Quantum Scattering Modelsmentioning
confidence: 99%
“…In ref. 35, diffraction data from neon displayed in Fig. 7 and 8 were compared with a recent ab initio calculation of the PEL by Miraglia and Gravielle 79 who kindly accepted to provide a compact description of their results in the form of effective binary interaction potentials.…”
Section: Quantitative Comparison With Quantum Theorymentioning
confidence: 99%
“…79 optimized to the data by a new close coupling code 106 providing the first quantitative agreement. 35 vibrational transition can be calculated exactly as p e = |hc|e idkz |ci| 2 which, for an atom initially in the vibrational ground state is proportional to p e p e ÀEr/h oD (eqn (3)). This probability is significant only when the recoil energy is less than a vibrational energy quantum 21 and can be identified as the Mössbauer-Lamb-Dicke probability for recoil-less photon emission characteristic of a trapped atom, for instance in an optical lattice.…”
Section: Quantum Binary Scatteringmentioning
confidence: 99%
“…Experimentally, a combined GIFAD and HAS study of a thin overlayer, for instance of graphene, 100 would probably help in the identification of specific vibration modes and allow significant progress. Regarding elastic diffraction, the recent progress 35 should allow for the implementation of a crystallographic software starting with a qualitative adjustment of surface atoms coordinates and effective binary interaction potentials by the HCW model and then final quantitative optimization by quantum scattering programs.…”
In the elastic regime, GIFAD is equivalent to TEAS with an effective energy E⊥ between 1 meV and 1 eV providing a high sensitivity to topology and to attractive forces. The inelastic regime merges to the classical limit and is still in development.
“…The effect of 85 the attractive part of the potential onto the incident He atom can be seen as an analogy to refraction for classical scattering from an isolated target. Since only the z-component is important, refraction can also be made visible in the case of fast Ne atoms, if angles close to grazing incidence are used 24 .…”
Section: The Atom-surface Interaction Potentialmentioning
Gas-surface scattering experiments yield high accuracy interaction potentials in the van der Waals regime. A perspective overview for topological semimetals & insulators is provided and the importance for benchmarking ab initio calculations outlined.
Grazing incidence fast atom diffraction at crystal surface (GIFAD or FAD) have demonstrated coherent diffraction both at effective energies close to one eV ($\lambda_\perp\approx$ 14 pm) and at elevated surface...
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