The CLAS12 drift chamber system

The CEBAF Large Acceptance Spectrometer at 12 GeV (CLAS12) is located in Hall B, one of the experimental halls at Jefferson Lab. The forward part of CLAS12 is built around a superconducting toroidal magnet. The six coils of the toroid divide the detector azimuthally into six sectors. Each sector con...

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Veröffentlicht in:Nuclear instruments & methods in physics research. Section A, Accelerators, spectrometers, detectors and associated equipment Accelerators, spectrometers, detectors and associated equipment, 2020-04, Vol.959 (C), p.163518, Article 163518
Hauptverfasser: Mestayer, M.D., Adhikari, K., Bennett, R.P., Bueltmann, S., Chetry, T., Christo, S.B., Cook, M., Cuevas, R.C., Dodge, G.E., El Fassi, L., Forest, T.A., Jacobs, G., Hartlove, T., Hayward, T.B., Kabir, L., Kuhn, S.E., McNulty, D., Nanda, S., Newton, J., Taylor, W.M., Weinstein, L.B., Ziegler, V.
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Sprache:eng
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Zusammenfassung:The CEBAF Large Acceptance Spectrometer at 12 GeV (CLAS12) is located in Hall B, one of the experimental halls at Jefferson Lab. The forward part of CLAS12 is built around a superconducting toroidal magnet. The six coils of the toroid divide the detector azimuthally into six sectors. Each sector contains three multi-layer drift chambers for reconstructing the trajectories of charged particles originating from a fixed target. Each of the 18 planar chambers has two “superlayers” of six layers each, with the wires in the two adjacent superlayers oriented at ±6° stereo angles. Each layer has 112 hexagonal cells spanning a range from about 5° to 40° in polar angle. The six-layer structure provides redundancy in track segment finding and good tracking efficiency even in the presence of some individual wire inefficiency. The design, construction, operation, and calibration methods are described, and estimates of the efficiency and resolution are presented from in-beam measurements.
ISSN:0168-9002
1872-9576
DOI:10.1016/j.nima.2020.163518