1978
DOI: 10.1088/0022-3719/11/8/015
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Interionic potentials for alkali halides. II. Completely crystal independent specification of Born-Mayer potentials

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Cited by 215 publications
(73 citation statements)
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“…The first term gives the longrange electrostatic interaction, and the second one represents the short-range Buckingham type interaction 58 : parameters for all ionic pairs were obtained from previous studies [59][60][61] and are listed in Supplementary Table 4. It should be mentioned that the short-range interaction between two Br À ions is neglected since only one Br À ion is present in the simulation at any time.…”
Section: Articlementioning
confidence: 99%
“…The first term gives the longrange electrostatic interaction, and the second one represents the short-range Buckingham type interaction 58 : parameters for all ionic pairs were obtained from previous studies [59][60][61] and are listed in Supplementary Table 4. It should be mentioned that the short-range interaction between two Br À ions is neglected since only one Br À ion is present in the simulation at any time.…”
Section: Articlementioning
confidence: 99%
“…This approach allows us to include the influence of applied bias on the forces and atomic geometries. Interatomic interactions in the surface are included via fitted Buckingham potentials [51][52][53][54]. As the tip is contacted to the surface, we expect the apex to be covered by LiF and model it as a simple dipole [45,55,56]-since we are interested in the interactions at LR, an atomistic model of the tip is unnecessary.…”
Section: Prl 109 146101 (2012) P H Y S I C a L R E V I E W L E T T Ementioning
confidence: 99%
“…where q i are the ion charges, r ij is the distance between ionic pairs and A ij , B ij , and ρ ij are parameters defined for 31 The parameters for all ionic pairs were obtained from previous studies [32][33][34] and are listed in Tables I and II. The software is specifically designed to simulate a system consisting of a surface and an atomic force microscopy (AFM) tip, and to mimic the motion of the tip in a real AFM experiment. In this particular case the tip was forced to oscillate harmonically above the surface as in a DFM/DFS experiment: The oscillation amplitude was set to match the experimental value of 1 nm, but the frequency was increased to 100 MHz in order to reduce the simulation time and make it affordable.…”
Section: Simulation Detailsmentioning
confidence: 99%