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  • The CLAS12 superconducting ...
    Fair, R.; Baltzell, N.; Bachimanchi, R.; Biallas, G.; Burkert, V. D.; Campero-Rojas, P.; Elementi, L.; Elouadrhiri, L.; Eng, B.; Ghoshal, P. K.; Hogan, J.; Insley, D.; Kashikhin, V.; Kashy, D.; Krave, S.; Kumar, O.; Laney, M.; Legg, R.; Lagerquist, V.; Lester, M.; Lemon, T.; Lung, A.; Luongo, C.; Matalevich, J.; Mestayer, M. D.; Miller, R.; Moore, W.; Newton, J.; Nobrega, F.; Pastor, O.; Philip, S.; Rajput-Ghoshal, R.; Rao Ganni, V.; Rode, C.; Sandoval, N.; Spiegel, S.; Tilles, D.; Tremblay, K.; Velev, G.; Wilson, C.; Wiseman, M.; Young, G. R.

    Nuclear instruments & methods in physics research. Section A, Accelerators, spectrometers, detectors and associated equipment, 05/2020, Letnik: 962, Številka: C
    Journal Article

    As part of the Jefferson Lab 12 GeV upgrade, the Hall B CLAS12 system requires two superconducting iron-free magnets — a torus and a solenoid. The physics requirements to maximize space for the detectors guided engineers toward particular coil designs for each of the magnets which, in turn, led to the choice of using conduction cooling. The torus consists of 6 trapezoidal NbTi coils connected in series with an operating current of 3770 A. The solenoid is an actively shielded 5 T magnet consisting of 5 NbTi coils connected in series operating at 2416 A. Within the hall, the two magnets are located in close proximity to each other and are completely covered both inside and outside by particle detectors. Stringent size limitations were imposed for both magnets and introduced particular design and fabrication challenges. This paper describes the design, construction, installation, commissioning, and operation of the two magnets.