Abstract
Al thin films were deposited at 873 K on a Re(101̄0) surface and examined by means of low-energy electron diffraction (LEED), Auger electron spectroscopy (AES), thermal desorption spectroscopy (TDS), and work function (ΔΦ) measurements. In the submonolayer range (0< Θ Al<0.6), we find two Al LEED structures, a p(3 × 1) at Θ Al ≈ 0.3, and a p(2 × 1) at Θ Al ≈ 0.5. In the same coverage range, a single TD state denoted as β 3 appears having a desorption energy of 440 kJ/mol. Close to Θ Al ≈ 1 another (2 × 1) LEED phase and a second TD state ( β 2) develop which exhibits a desorption energy of ∼ 375 kJ/mol. This (2 × 1) phase is then replaced up to Θ Al ≈ 2 by a clear c(2 × 2) phase, followed by a p(2 × 2) and another c(2 × 2) structure at still higher Al coverages. In this multilayer range, the TD spectra are dominated by a single desorption state denoted as β 1 which reflects a fractional-order kinetics and yields an activation energy of ∼ 345 kJ/mol. The deposition of Al reduces the Re work function by ∼ 1.2 eV. A plot of the Re versus Al Auger intensity reveals a clear break at Θ Al ≈ 1 and a less pronounced break around Θ Al ≈ 2, while for higher Al coverages the Re AES intensity decays unspecifically, which suggests deviations from a plain layer-by-layer growth. Up to ∼ 8 deposited monolayers the structure of the Al film is determined by the crystallography of the Re(101̄0) surface and by relaxation processes to overcome the misfit.
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.