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- W1999269747 abstract "Radiofrequency (rf) waves can accelerate electrons into material boundaries, so that electron confinement requires rf sheath potentials that are significantly larger than the thermal Bohm sheath. The condition for rf sheaths to occur is that the rf electric field has a component E|| parallel to the equilibrium magnetic field. Thus, a proper treatment of rf wave propagation requires an accurate description of the geometry of the magnetic field and of the bounding surfaces, and a boundary condition (BC) that includes the effect on the waves of the electron-poor sheath. When the static magnetic field has a component at an angle to the sheath, the propagating fast wave (with E||=0) is coupled to a slow wave (with E||≠0) in order to satisfy the boundary condition at the metal wall, and the time-averaged sheath potential has a strong component from rectification of the rf sheath. In this brief communication, a previously derived sheath BC is reformulated to treat the coupling of the fast wave to the slow wave analytically, thereby greatly reducing the necessary numerical resolution required for calculation of fast wave propagation." @default.
- W1999269747 created "2016-06-24" @default.
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- W1999269747 date "2012-03-01" @default.
- W1999269747 modified "2023-10-16" @default.
- W1999269747 title "A sheath boundary condition for fast wave propagation near conducting surfaces" @default.
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- W1999269747 doi "https://doi.org/10.1063/1.3692734" @default.
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