2016
DOI: 10.1016/j.nima.2016.03.115
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Measurement and tricubic interpolation of the magnetic field for the OLYMPUS experiment

Abstract: The OLYMPUS experiment used a 0.3 T toroidal magnetic spectrometer to measure the momenta of outgoing charged particles. In order to accurately determine particle trajectories, knowledge of the magnetic field was needed throughout the spectrometer volume. For that purpose, the magnetic field was measured at over 36,000 positions using a three-dimensional Hall probe actuated by a system of translation tables. We used these field data to fit a numerical magnetic field model, which could be employed to calculate … Show more

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Cited by 14 publications
(17 citation statements)
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References 11 publications
(11 reference statements)
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“…Alternating beams of electrons and positrons in the DORIS storage ring were passed through a windowless unpolarized hydrogen target that was internal to the ring vacuum [15]. The OLYMPUS spectrometer [13] consisted of two instrumented sectors of an 8-coil toroid magnet [16] surrounding the target, shown in Fig. 1 right.…”
Section: The Olympus Experimentsmentioning
confidence: 99%
“…Alternating beams of electrons and positrons in the DORIS storage ring were passed through a windowless unpolarized hydrogen target that was internal to the ring vacuum [15]. The OLYMPUS spectrometer [13] consisted of two instrumented sectors of an 8-coil toroid magnet [16] surrounding the target, shown in Fig. 1 right.…”
Section: The Olympus Experimentsmentioning
confidence: 99%
“…unpolarized hydrogen target that was internal to the ring vacuum [19]. The OLYMPUS spectrometer [17] consisted of two instrumented sectors of an 8-coil toroid magnet [20] surrounding the target, shown in Fig. 2 left.…”
Section: The Olympus Experimentsmentioning
confidence: 99%
“…Walls of time-of-flight scintillator paddles provided a trigger signal for the tracking detectors and rough particle identification information, while large-acceptance drift chambers permitted exclusive reconstruction of leptons and protons trajectories from elastic scattering events. The lepton beam species was alternated daily to control long-period systematic effects on the measurement of the e + p and e − p cross sections, and the detector positions and magnetic field were surveyed in detail to properly account for the acceptance differences for e + p and e − p events [29]. Using the precise survey of the detector system and magnetic field in conjunction with a newly written generator for radiative e ± p events [26,30], a detailed Geant4 [31] simulation was developed to account for the effects of non-hard TPE lepton charge odd effects as well as the detector acceptance and efficiency.…”
Section: The Olympus Experimentsmentioning
confidence: 99%