Each of the two slow-extracted proton beams of the CERN 400 GeV Super Proton Synchrotron can be d... more Each of the two slow-extracted proton beams of the CERN 400 GeV Super Proton Synchrotron can be divided into three parts by means of steel- septum magnets for the simultaneous irradiation of up to three production targets. The magnets have radiation-proof coils, integrated vacuum chambers and 'plug-in' connections. The paper describes the design of the magnets and gives the results of the magnetic field measurements. (3 refs)
Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 1985
A simple almost non-destructive device has been built to accurately measure the transverse emitta... more A simple almost non-destructive device has been built to accurately measure the transverse emittances of the proton and antiproton beams in the CERN SPS collider. A fine wire passing rapidly through the beams acts as a target for the production of high energy secondary ...
Each of the two slow-extracted proton beams of the CERN 400 GeV Super Proton Synchrotron can be d... more Each of the two slow-extracted proton beams of the CERN 400 GeV Super Proton Synchrotron can be divided into three parts by means of steel- septum magnets for the simultaneous irradiation of up to three production targets. The magnets have radiation-proof coils, integrated vacuum chambers and 'plug-in' connections. The paper describes the design of the magnets and gives the results of the magnetic field measurements. (3 refs)
Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 1985
A simple almost non-destructive device has been built to accurately measure the transverse emitta... more A simple almost non-destructive device has been built to accurately measure the transverse emittances of the proton and antiproton beams in the CERN SPS collider. A fine wire passing rapidly through the beams acts as a target for the production of high energy secondary ...
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