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Jump processes in surface diffusion - Bilkent University - Faculty of ...

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58 G. Antczak, G. Ehrlich / Surface Science Reports 62 (2007) 39–61<br />

Fig. 60. Schematic <strong>of</strong> different types <strong>of</strong> jump <strong>processes</strong> for an adatom on<br />

W(211) [126]. β R denotes rebound transition.<br />

Fig. 58. Normal Arrhenius plot for β double jumps <strong>of</strong> W adatom on<br />

W(211) [126].<br />

Fig. 61. Rate <strong>of</strong> rebound jumps, obta<strong>in</strong>ed as the difference between the<br />

sum <strong>of</strong> s<strong>in</strong>gle plus double jumps and total jump rate extrapolated from low<br />

temperatures [129].<br />

Fig. 59. Arrhenius plot for the sum <strong>of</strong> all jump rates measured for W adatom<br />

on W(211). For temperatures ≥310 K, rate falls below l<strong>in</strong>ear plot [126].<br />

such a rebound transition, and it is therefore not detected <strong>in</strong><br />

the normal <strong>diffusion</strong> measurements, but rebounds were found <strong>in</strong><br />

molecular dynamics simulations <strong>in</strong> 1989 by DeLorenzi [127],<br />

and a few years later by Sanders and DePristo [128] and Ferrón<br />

et al. [113].<br />

A way to measure such rebounds has recently been<br />

discovered. Antczak [129] has po<strong>in</strong>ted out that the sum <strong>of</strong> the<br />

measured jump rates has to be subtracted from the straightl<strong>in</strong>e<br />

Arrhenius plot obta<strong>in</strong>ed by extrapolat<strong>in</strong>g the sum from<br />

low temperatures. The rebound rate so obta<strong>in</strong>ed is shown<br />

<strong>in</strong> Fig. 61; it has an activation energy <strong>of</strong> 1.03 ± 0.06 eV<br />

and a frequency prefactor <strong>of</strong> 1.40(×10.3 ±1 ) × 10 16 s −1 , and<br />

thus lies midway between s<strong>in</strong>gle and double jumps. What<br />

is surpris<strong>in</strong>g is that rebounds were not detected <strong>in</strong> twodimensional<br />

<strong>diffusion</strong> on W(110) at all, suggest<strong>in</strong>g it may be an<br />

effect tied to the channelled structure <strong>of</strong> W(211) that is <strong>in</strong>volved<br />

<strong>in</strong> these transitions. However, they have been seen previously <strong>in</strong><br />

simulations <strong>of</strong> self-<strong>diffusion</strong> on the Cu(111) plane [113].<br />

It should be noted that long jumps are not limited to the<br />

movement <strong>of</strong> s<strong>in</strong>gle atoms. As is apparent from Fig. 62,<br />

long jumps were observed by Wang [130,131] for clusters <strong>of</strong><br />

iridium atoms on Ir(111), and for the large organic molecules<br />

decacyclene and hexa-tert-butyl-decacyclene by Schunack<br />

et al. [132]. However, <strong>in</strong>formation about the k<strong>in</strong>etics <strong>of</strong> these<br />

<strong>processes</strong> is limited and cry<strong>in</strong>g for more work.<br />

F<strong>in</strong>ally, it should be said that theoretical predictions about<br />

long jumps have been very important <strong>in</strong> po<strong>in</strong>t<strong>in</strong>g to their<br />

contributions <strong>in</strong> <strong>diffusion</strong>. However, even the limited number<br />

<strong>of</strong> experiments done so far have already revealed that these<br />

transitions are rather more varied and more significant than<br />

predicted, especially at low temperatures.<br />

4. Summary<br />

This survey should make it clear that a whole variety <strong>of</strong><br />

different jumps contributes to <strong>surface</strong> <strong>diffusion</strong> on metals. Atom<br />

exchange <strong>processes</strong> are <strong>of</strong> course very much affected by the<br />

chemistry <strong>of</strong> the <strong>in</strong>teract<strong>in</strong>g partners, but have so far only<br />

been observed <strong>in</strong> experiments with fcc metals. On channelled<br />

<strong>surface</strong>s the direction favoured <strong>in</strong> <strong>diffusion</strong> is still puzzl<strong>in</strong>g.

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