Developing the technique of measurements of magnetic field in the CMS steel yoke elements with flux-loops and Hall probes

• Published in: IEEE transactions on nuclear science Vol. 51; no. 5; pp. 2187 - 2192
• Main Authors: Klyukhin, V.I., Campi, D., Cure, B., Gaddi, A., Gerwig, H., Grillet, J.P., Herve, A., Loveless, R., Smith, R.P.
• Format: Journal Article
• Language: English
• Published: New York IEEE 01.10.2004; The Institute of Electrical and Electronics Engineers, Inc. (IEEE)
• Subjects: Collision mitigation; Detectors; Hall effect devices; Large Hadron Collider; Magnetic field measurement; Magnetic fields; Magnetic sensors; Magnetism; Solenoids; Steel; Superconducting magnets; Testing
• ISSN: 0018-9499; 1558-1578
• DOI: 10.1109/TNS.2004.834722

Compact muon solenoid (CMS) is a general-purpose detector designed to run at the highest luminosity at the CERN large hadron collider (LHC). Its distinctive features include a 4 T superconducting solenoid with 6 m diameter by 12.5 m long free bore, enclosed inside a 10000-ton return yoke made of construction steel. Accurate characterization of the magnetic field everywhere in the CMS detector, including the large ferromagnetic parts of the yoke, is required. To measure the field in and around ferromagnetic parts, a set of flux-loops and Hall probe sensors will be installed on several of the steel pieces. Fast discharges of the solenoid during system commissioning tests will be used to induce voltages in the flux-loops that can be integrated to measure the flux in the steel at full excitation of the solenoid. The Hall sensors will give supplementary information on the axial magnetic field and permit estimation of the remanent field in the steel after the fast discharge. An experimental R&D program has been undertaken, using a test flux-loop, two Hall sensors, and sample disks made from the same construction steel used for the CMS magnet yoke. A sample disc, assembled with the test flux-loop and the Hall sensors, was inserted between the pole tips of a dipole electromagnet equipped with a computer-controlled power supply to measure the excitation of the steel from full saturation to zero field. The results of the measurements are presented and discussed.