True 3-D displays for avionics and mission crewstations
Elizabeth A. Sholler, Frederick M. Meyer, et al.
SPIE AeroSense 1997
A computational method is described, which, starting from given difraction intensities, approaches effectively the best-fit corrugation function ζ(R). Because of the approximations involved, the procedure works well for smooth corrugations with amplitudes not exceeding ∼10% of the lattice constant. The method rests on two crucial observations: (i) With the full knowledge of the scattering amplitudes AG = |AG|exp(iθ{symbol}G) (absolute values plus phases), the corrugation function can be calculated to a high degree of accuracy from ζ(R) = (2iki)-1 In |-ΣAG exp(iG·R)| which is derived easily from the hard corrugated wall scattering (HCWS) equation by approximating kG by -ki (ki and kG being the wavevectors of the incoming and diffracted beams, respectively), (ii) With only the |AG|'s (or intensities) known, approximate solutions of the HCWS equation can be obtained with a rough estimate of the relative phases of only a few intense diffraction beams; the estimate is readily performed by investigating systematically a coarse mesh of phases. In this way, approximate corrugations are found with which a full set of phases can be generated, which allows the calculation of an improved ζ(R); this step is repeated in a loop, until optimum agreement between calculated and given intensities is obtained. The effectiveness of the procedure is demonstrated for three one-dimensional model corrugations described by several Fourier coefficients. The method is finally applied to the case of H2 diffraction from the quasi-one-dimensional adsorbate corrugation Ni(110) + H(1 × 2). © 1981.
Elizabeth A. Sholler, Frederick M. Meyer, et al.
SPIE AeroSense 1997
Zelek S. Herman, Robert F. Kirchner, et al.
Inorganic Chemistry
Joy Y. Cheng, Daniel P. Sanders, et al.
SPIE Advanced Lithography 2008
A. Nagarajan, S. Mukherjee, et al.
Journal of Applied Mechanics, Transactions ASME