Abstract
The deflection angle θ of a cathode‐ray beam accelerated by a potential V is shown to be proportional to the linear charge density ρ transverse to the beam on the interior of the electrostatic deflection system, θ=ρ/2Vε0. The voltage deflection sensitivity depends on the plate‐to‐plate capacitance c per unit width, θ/E=c/2Vε0. This includes edge effects and permits a determination of the sensitivity from capacitance measurements or a simple graphical evaluation from the dimensions of the deflection system. The use of parallel‐wire lines as a deflection system is suggested, and its deflection sensitivity evaluated. Such lines have low transit time error and are either easily tuned, or can be operated non‐resonant with resistive termination.

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