AVS 55th International Symposium & Exhibition
    Surface Science Thursday Sessions
       Session SS1-ThM

Paper SS1-ThM4
Optical Anisotropy Induced by Oblique Incidence Ion Bombardment of Ag(001)

Thursday, October 23, 2008, 9:00 am, Room 207

Session: Growth and Etching on Surfaces
Presenter: H. Wormeester, University of Twente, The Netherlands
Authors: H. Wormeester, University of Twente, The Netherlands
F. Everts, University of Twente, The Netherlands
B. Poelsema, University of Twente, The Netherlands
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Oblique incidence ion sputtering has become a widely used method for the creation of highly regular patterns of lines and dots. On a Ag(001) surface oblique incidence sputtering creates a ripple pattern that exhibits plasmonic features. The photon energy of this plasmonic feature depends on the ripple periodicity. The development of these anisotropic features is measured in-situ with the optical technique Reflection Anisotropy Spectroscopy (RAS). The ion induced nanopatterns are prepared using 2 keV Ar ions with a flux of a few Μa/cm2 in a temperature range of 300 - 420K. With RAS, a periodicity of ripples above 200 nm is measured by a shift in photon energy of the plasmon resonance. Features with a smaller periodicity show a plasmon resonance around 3.65 Ev. For very grazing incidence sputtering, 80° polar angle of incidence, only a resonance feature around 3.65 Ev is observed. High resolution LEED measurements after sputtering confirm the formation of 1D nanoripples. For a polar angle of incidence of the ion beam of 70° a shift in the maximum of the plasmon resonance feature is observed. These spectra can be well described within the Rayleigh-Rice description for scattering from a slightly rough surface. The formation of nanoripples, i.e. a 1D roughening of the surface perpendicular to the direction of the ion beam, suffices to describe the measured optical data. The evolution of the rms, wavelength and wavelength distribution of the ion bombardment induced nanoripples is obtained from in-situ measurements. For a polar angle of the ion beam of 61° we find that also the roughening in the direction along the nanorippels has to be taken into account to describe the optical spectra.