The dynamics of collision-induced desorption (CID) of N-2 from Ru(001)
exposed to hyperthermal rare gas colliders generated in a supersonic
atomic beam source have been studied. Low coverage of 0.01 ML N-15(2)
at crystal temperature of 96 K was chosen to represent a CID process o
f a practically isolated molecule, neglecting the effect of lateral N-
2-N-2 interactions. The cross sections for CID of nitrogen molecules,
sigma(des)(E-i, theta(i)), as a function of the kinetic energy and ang
le of incidence of Ar and Kr colliders have been measured. It was foun
d that sigma(des)(E-i, theta(i)=0 degrees) changes monotonically in th
e range 0-25 Angstrom(2) for beam energy in the range of 0.5-5.5 eV an
d is insensitive to the type of collider (Ar, Kr) as well as to the ad
sorbate isotope (N-14(2), N-15(2)). The threshold energy for desorptio
n has been determined to be 0.50+/-0.10 eV, which is twice the binding
energy of N-2 to Ru(001). The cross section for CID at a fixed collid
er's energy rises approximately four times as the incidence angle thet
a(i) increases from 0 degrees to 70 degrees relative to the surface no
rmal. Neither normal nor total energy scaling of the cross section cou
ld describe the results. The sigma(des)(theta(i)) scales reasonably we
ll, however, with the tangential energy of the collider for angles abo
ve 30 degrees. Classical molecular dynamics simulations were performed
to gain better understanding of the CID process. Threshold energy and
angular dependence of the cross section were reproduced very well. Th
e predominant CID mechanism was concluded to originate from a direct r
are gas-nitrogen collision, in which impulsive-bending and the motion
along the surface are coupled to the adsorbate motion which leads to d
esorption. (C) 1998 American Institute of Physics. [S0021-9606(98)0102
0-4].