TY - JOUR
T1 - Transport issues in focused electron beam chemical vapor deposition
AU - Fedorov, Andrei G.
AU - Rykaczewski, Konrad
AU - White, William B.
N1 - Funding Information: NSF Grant DMI 0403671 provided financial support for this work via NIRT Program on EB-CVD. We also thank Drs. T. Orlando and J. Lackey for useful comments. Copyright: Copyright 2008 Elsevier B.V., All rights reserved.
PY - 2007/9/25
Y1 - 2007/9/25
N2 - In this contribution we critically review heat and mass transfer issues in the Focused Electron Beam Chemical Vapor Deposition (FEB-CVD). In general, the transport of both the precursor molecules and the primary/secondary electrons facilitate nanostructure deposition. Depending on the operating pressure either continuous advection-diffusion mass conservation equation or the kinetic Boltzmann Transport Equation (BTE) describes the transport of precursor molecules to the substrate surface. At the surface, some of the precursor molecules are adsorbed, spatially re-distributed by surface diffusion, and, finally, a fraction of the adsorbed molecules become converted into a solid deposit. This occurs upon interaction with back-scattered primary electrons and secondary electrons, yielded by the substrate and deposit upon impingement of the high-energy primary electron beam. The interactions of the primary electrons with the substrate and nanoscale-confined deposit possibly induce significant localized heating. Such energy transfer process is complex, involves non-classical heat conduction, and may greatly influence the deposition process. The pertinent question is then what controls the FEB-CVD process, i.e., both time dependent growth of the nanostructure and its shape evolution? The answer to this question can be obtained via complimentary theoretical and experimental studies, discussed here with the main focus on transport phenomena underlying FEB-CVD.
AB - In this contribution we critically review heat and mass transfer issues in the Focused Electron Beam Chemical Vapor Deposition (FEB-CVD). In general, the transport of both the precursor molecules and the primary/secondary electrons facilitate nanostructure deposition. Depending on the operating pressure either continuous advection-diffusion mass conservation equation or the kinetic Boltzmann Transport Equation (BTE) describes the transport of precursor molecules to the substrate surface. At the surface, some of the precursor molecules are adsorbed, spatially re-distributed by surface diffusion, and, finally, a fraction of the adsorbed molecules become converted into a solid deposit. This occurs upon interaction with back-scattered primary electrons and secondary electrons, yielded by the substrate and deposit upon impingement of the high-energy primary electron beam. The interactions of the primary electrons with the substrate and nanoscale-confined deposit possibly induce significant localized heating. Such energy transfer process is complex, involves non-classical heat conduction, and may greatly influence the deposition process. The pertinent question is then what controls the FEB-CVD process, i.e., both time dependent growth of the nanostructure and its shape evolution? The answer to this question can be obtained via complimentary theoretical and experimental studies, discussed here with the main focus on transport phenomena underlying FEB-CVD.
KW - Electron beam CVD
KW - Heat and mass transfer
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U2 - 10.1016/j.surfcoat.2007.04.031
DO - 10.1016/j.surfcoat.2007.04.031
M3 - Article
SN - 0257-8972
VL - 201
SP - 8808
EP - 8812
JO - Surface and Coatings Technology
JF - Surface and Coatings Technology
IS - 22-23 SPEC. ISS.
ER -