Double Scattering of High-Energy Protons by Hydrogen and Carbon
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Abstract
Measurements have been made of the asymmetry in the second scattering of protons first scattered from an internal target in the 240-Mev proton beam of the cyclotron. Referring to Fig. 1, protons scattered at 27° are collimated, selected roughly in energy, and pass into a second-scattering apparatus outside the cyclotron vacuum tank. This apparatus is rigidly mounted in a cylindrical can rotatable about an axis which can be made to coincide with the direction of the protons from target I. The useful beam is defined by a cylindrical scintillation counter on the axis. Further, with a polyethylene second target a p—p scatter is detected by quadruple coincidence among the beam defining counter, a two-counter telescope detecting the protons scattered into a range about 27°, and a counter for the low-energy recoil. An exploratory counter 15 inches behind the beam-defining counter is used in coincidence with it to align the beam with the mechanical axis of the can to better than 0.4°. The beam spread determined by this method is 2° and is approximately symmetric. Target II is $\frac{2}{3}$ the diameter of the beam-defining counter, and both are optically set on axis. As expected from these dimensions, the quadruple rate was insensitive to small displacements of the second target from the axis.
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