Modeling Micro-Porous Surfaces for Secondary Electron Emission Control to Suppress Multipactor

This work seeks to understand how the topography of a surface can be engineered to control secondary electron emission (SEE) for multipactor suppression. Two unique, semi-empirical models for the secondary electron yield (SEY) of a micro-porous surface are derived and compared. The first model is based on a two-dimensional (2D) pore geometry. The second model is based on a three-dimensional (3D) pore geometry. The SEY of both models is shown to depend on two categories of surface parameters: chemistry and topography. An important parameter in these models is the probability of electron emissions to escape the surface pores. This probability is shown by both models to depend exclusively on the aspect ratio of the pore (the ratio of the pore height to the pore diameter). The increased accuracy of the 3D model (compared to the 2D model) results in lower electron escape probabilities with the greatest reductions occurring for aspect ratios less than two. In order to validate these models, a variety of micro-porous gold surfaces were designed and fabricated using photolithography and electroplating processes. The use of an additive metal-deposition process (instead of the more commonly used subtractive metal-etch process) provided geometrically ideal pores which were necessary to accurately assess the 2D and 3D models. Comparison of the experimentally measured SEY data with model predictions from both the 2D and 3D models illustrates the improved accuracy of the 3D model. For a micro-porous gold surface consisting of pores with aspect ratios of two and a 50% pore density, the 3D model predicts that the maximum total SEY will be one. This provides optimal engineered surface design objectives to pursue for multipactor suppression using gold surfaces

Energy loss of fragment protons dissociated from 0.2- and 0.5-MeV/amu H2+ ions incident in carbon foils

Energy losses of fragment protons from 0.2- and 0.5-MeV/amu H2+ were measured at transmission through amorphous carbon foils of thickness less than 25μg/cm2. The energy losses of randomly oriented fragment protons and those of the fragment protons aligned in the direction of motion show how the spatial correlation of the protons affects the energy loss. We use the dielectric formalism to calculate the stopping power of amorphous carbon for two spatially correlated protons and compare with the experimental energy-loss data. We conclude that higher energies or thinner foils are necessary to understand the anomalous energy loss of aligned proton pairs.Financial support provided to R.G.-M. and I.A. from the Spanish Dirección General de Enseñanza Superior (Project No. PB96-1118) and the Generalitat Valenciana (Project No. GV99-54-1-01)