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Aca - Departamento de Física - Universidad Técnica Federico Santa ...

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V Encuentro Sud Americano <strong>de</strong> Colisiones Inelásticas en la Materia<br />

Fast atom diffraction from metallic surfaces<br />

M.S. Gravielle 1 , G. Bocán 2 , and R. Díez Muiño 3<br />

1 Instituto <strong>de</strong> Astronomía y <strong>Física</strong> <strong>de</strong>l Espacio, CONICET, Bs. As, Argentina, and Depto <strong>de</strong> <strong>Física</strong>,<br />

FCEN, UBA.<br />

2 Centro Atómico Bariloche, CNEA and CONICET, S.C. <strong>de</strong> Bariloche, Río Negro, Argentina.<br />

3 Donostia International Physics Center (DIPC) and C. Fís. Materiales CSIC-UPV/EHU, San Sebastián,<br />

Spain.<br />

E-mail: msilvia@iafe.uba.ar<br />

1. INTRODUCTION<br />

Diffraction from crystal surfaces produced by<br />

grazing scattering of atoms in the keV energy<br />

range is nowadays attracting consi<strong>de</strong>rable attention.<br />

The first experimental evi<strong>de</strong>nces of this<br />

effect were reported for insulator surfaces [1] for<br />

which the presence of a band gap strongly suppresses<br />

inelastic electronic processes, favoring<br />

the conservation of quantum coherence. However,<br />

this diffraction effect has recently been<br />

observed at metallic materials [2,3] as well, although<br />

electron excitations were supposed to<br />

smudge interference signatures for these surfaces.<br />

The aim of this work is to study the<br />

atomic diffraction from metal surfaces by consi<strong>de</strong>ring<br />

keV nitrogen atoms impinging grazingly<br />

on Ag(111) .<br />

2. THEORETICAL MODEL<br />

To <strong>de</strong>scribe the scattering process we employ<br />

a distorted-wave mo<strong>de</strong>l - the surface-eikonal<br />

approximation [4] - that makes use of the eikonal<br />

wave function to represent the elastic collision<br />

with the surface, while the movement of the<br />

fast projectile is <strong>de</strong>scribed classically by consi<strong>de</strong>ring<br />

axially channeled trajectories for different<br />

initial conditions. The surface-eikonal T-matrix<br />

element reads:<br />

r r<br />

(eik)<br />

Tif<br />

= ∫ dRos<br />

aif<br />

( Ros<br />

),<br />

(1)<br />

where R r<br />

<strong>de</strong>termines the initial position of the<br />

os<br />

projectile on the surface plane and<br />

a<br />

if<br />

r<br />

( R<br />

os<br />

r<br />

-3<br />

) = ( 2π)<br />

∫ dt |vz<br />

( RP<br />

) |×<br />

r r r<br />

exp[ -iQ.R -i η(<br />

R )] V<br />

P<br />

P<br />

SP<br />

r<br />

( R<br />

P<br />

)<br />

(2)<br />

is the transition amplitu<strong>de</strong> associated with the<br />

r r<br />

classical path RP<br />

( Ros<br />

, t)<br />

, with Q r the projectile<br />

r<br />

momentum transfer and v z<br />

( RP<br />

) the component<br />

of the projectile velocity perpendicular to the<br />

surface plane. In Eq. (2), η ( R<br />

r P<br />

) is the eikonal-<br />

Maslov phase that takes into account the action<br />

of the projectile-surface potential V ( R<br />

r<br />

SP P)<br />

along<br />

the classical path.<br />

An accurate potential energy surface for the<br />

N/Ag(111) system was <strong>de</strong>rived from <strong>de</strong>nsity<br />

functional theory (DFT) calculations as implemented<br />

in the "Vienna Ab-initio Simulation<br />

Program" (VASP) co<strong>de</strong> [5], combined with an<br />

elaborate interpolation method [6].<br />

3. RESULTS<br />

We apply the theoretical mo<strong>de</strong>l to evaluate<br />

angular projectile distributions for impact along<br />

different low-in<strong>de</strong>x crystallographic directions.<br />

The influence of the inci<strong>de</strong>nce energy and the<br />

symmetry of the consi<strong>de</strong>red channel are both<br />

analyzed.<br />

32 Valparaíso, Chile

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