Abstract
A method for the calculation of the damping rate due to electron–hole pair excitation for atomic and molecular motion at metal surfaces is presented. The theoretical basis is provided by Time Dependent Density Functional Theory (TDDFT) in the quasi-static limit and calculations are performed within a standard plane-wave, pseudopotential framework. The artificial periodicity introduced by using a super-cell geometry is removed to derive results for the motion of an isolated atom or molecule, rather than for the coherent motion of an ordered over-layer. The algorithm is implemented in parallel, distributed across both k and g space, and in a form compatible with the CASTEP code. Test results for the damping of the motion of hydrogen atoms above the Cu(111) surface are presented.
| Original language | English |
|---|---|
| Pages (from-to) | 163-173 |
| Number of pages | 11 |
| Journal | Computer Physics Communications |
| Volume | 137 |
| Issue number | 1 |
| DOIs | |
| Publication status | Published - 2001 |
Bibliographical note
ID number: ISI:000168917300013Fingerprint
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