Rc. Munoz et al., Surface roughness and surface-induced resistivity of gold films on mica: Application of quantitative scanning tunneling microscopy, PHYS REV B, 62(7), 2000, pp. 4686-4697
We report measurements of the resistivity rho(T) of a gold film 70 nm thick
deposited on mica preheated to 300 degrees C in UHV, performed between 4 a
nd 300 K, and measurements of the surface topography of the same film perfo
rmed with a scanning tunneling microscope (STM). From the roughness measure
d with the STM we determine the parameters delta (rms amplitude) and xi (la
teral correlation length) corresponding to a Gaussian representation of the
average height-height autocorrelation function (ACF). We use the parameter
s delta and xi to calculate the quantum reflectivity R and the increase in
resistivity induced by electron-surface scattering on this film, according
to a modified version of the theory of Sheng, Xing, and Wang (mSXW) [Munoz
Et al., J. Phys.: Condens. Matter 11, L299 (1999)]. The mSXW theory is able
to select the appropriate scale of distance over which corrugations take p
lace, leading to R approximate to 1 for corrugations taking place over scal
es of distances that are long when compared to a few Fermi wavelength lambd
a(F) and R<1 for corrugations taking place over scales of distances that ar
e comparable to lambda(F) (to within an order of magnitude). The reflectivi
ty R determined by corrugations ocurring over a scale of distances comparab
le to lambda(F) approaches zero for a certain angle. The resistivity rho(T)
of the film increases by roughly a factor of 4 between 4 and 300 K, and so
does the bulk resistivity po(T) predicted by mSXW theory. With the paramet
ers delta and xi measured on our 70-nm film, we reproduced approximately th
e thickness and temperature dependence of the resistivity (between 3 and 30
0 K) of several gold films on mica reported by Sambles, Elsom, and Jarvis [
Philos. Trans. R. Sec. London, Ser. A 304, 365 (1982)], without using any a
dustable parameters. The results of this paper suggest that the relevant qu
antities controlling electron-surface scattering in continuous gold films o
f arbitrary thickness, are the parameters delta and xi describing the avera
ge ACF that characterizes the surface of the sample on a nanoscopic scale,
in agreement with the accepted view regarding the conductivity of ultrathin
films.