Abstract
The beam of electron linear accelerators has desirable geometric properties, but usually contains undesirable secondary particles and a relatively broad energy spectrum. In order to dispose of the secondary particles and, at the same time, establish control of the width of the energy spectrum, several magnetic deflection systems have been considered for the Stanford machines. Two such systems are described here, one of which has been adopted for three of the Stanford accelerators. Both systems are capable of translating the beam without energy dispersion.

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