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Determination of the bending field integral of the LEP spectrometer dipole
The LEP spectrometer performed calibrations of the beam energy in the 2000 LEP run, in order to provide a kinematical constraint for the W boson mass measurement. The beam was deflected in the spectrometer by a steel core dipole, and the bending angle was measured by Beam-Position Monitors on either...
Autores principales: | , , , , , , , , , , , |
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Lenguaje: | eng |
Publicado: |
2004
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1016/j.nima.2005.01.306 http://cds.cern.ch/record/799441 |
_version_ | 1780904722982502400 |
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author | Chritin, R Cornuet, D Dehning, Bernd Hidalgo, A Hildreth, M Kalbreier, Willi Leclère, P Mugnai, G Palacios, J Roncarolo, F Torrence, E Wilkinson, G |
author_facet | Chritin, R Cornuet, D Dehning, Bernd Hidalgo, A Hildreth, M Kalbreier, Willi Leclère, P Mugnai, G Palacios, J Roncarolo, F Torrence, E Wilkinson, G |
author_sort | Chritin, R |
collection | CERN |
description | The LEP spectrometer performed calibrations of the beam energy in the 2000 LEP run, in order to provide a kinematical constraint for the W boson mass measurement. The beam was deflected in the spectrometer by a steel core dipole, and the bending angle was measured by Beam-Position Monitors on either side of the magnet. The energy determination relies on measuring the change in bending angle when ramping the beam from a reference point at 50 GeV to an energy within the LEP W physics regime, typically 93 GeV. The ratio of integrated bending fields at these settings (approximately 1.18 Tm/0:64 Tm) must be known with a precision of a few 10-5. The paper reports on the field mapping measurements which were conducted to determine the bending integral under a range of excitation currents and coil temperatures. These were made in the laboratory before and after spectrometer operation, using a test-bench equipped with a moving arm, carrying an NMR probe and Hall probes, and in the LEP tunnel itself, with a mapping trolley inside the vacuum chamber. The mapping data are related to local readings supplied by fixed NMR probes in the dipole, and a predictive model developed which shows good consistency for all datasets within the estimated uncertainty, which is 14 x 10-5 for the moving arm, and 3 x 10-5 for the mapping trolley. Measurements are also presented of the field gradient inside the dipole, and of the environmental magnetic fields in the LEP tunnel. When applied to the spectrometer energy calibrations, the bending field model calculates the ratio of integrated fields with an estimated uncertainty of 1.5 x 10-5. |
id | cern-799441 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2004 |
record_format | invenio |
spelling | cern-7994412019-09-30T06:29:59Zdoi:10.1016/j.nima.2005.01.306http://cds.cern.ch/record/799441engChritin, RCornuet, DDehning, BerndHidalgo, AHildreth, MKalbreier, WilliLeclère, PMugnai, GPalacios, JRoncarolo, FTorrence, EWilkinson, GDetermination of the bending field integral of the LEP spectrometer dipoleAccelerators and Storage RingsThe LEP spectrometer performed calibrations of the beam energy in the 2000 LEP run, in order to provide a kinematical constraint for the W boson mass measurement. The beam was deflected in the spectrometer by a steel core dipole, and the bending angle was measured by Beam-Position Monitors on either side of the magnet. The energy determination relies on measuring the change in bending angle when ramping the beam from a reference point at 50 GeV to an energy within the LEP W physics regime, typically 93 GeV. The ratio of integrated bending fields at these settings (approximately 1.18 Tm/0:64 Tm) must be known with a precision of a few 10-5. The paper reports on the field mapping measurements which were conducted to determine the bending integral under a range of excitation currents and coil temperatures. These were made in the laboratory before and after spectrometer operation, using a test-bench equipped with a moving arm, carrying an NMR probe and Hall probes, and in the LEP tunnel itself, with a mapping trolley inside the vacuum chamber. The mapping data are related to local readings supplied by fixed NMR probes in the dipole, and a predictive model developed which shows good consistency for all datasets within the estimated uncertainty, which is 14 x 10-5 for the moving arm, and 3 x 10-5 for the mapping trolley. Measurements are also presented of the field gradient inside the dipole, and of the environmental magnetic fields in the LEP tunnel. When applied to the spectrometer energy calibrations, the bending field model calculates the ratio of integrated fields with an estimated uncertainty of 1.5 x 10-5.CERN-AB-2004-094CERN-PH-EP-2004-058oai:cds.cern.ch:7994412004-10-11 |
spellingShingle | Accelerators and Storage Rings Chritin, R Cornuet, D Dehning, Bernd Hidalgo, A Hildreth, M Kalbreier, Willi Leclère, P Mugnai, G Palacios, J Roncarolo, F Torrence, E Wilkinson, G Determination of the bending field integral of the LEP spectrometer dipole |
title | Determination of the bending field integral of the LEP spectrometer dipole |
title_full | Determination of the bending field integral of the LEP spectrometer dipole |
title_fullStr | Determination of the bending field integral of the LEP spectrometer dipole |
title_full_unstemmed | Determination of the bending field integral of the LEP spectrometer dipole |
title_short | Determination of the bending field integral of the LEP spectrometer dipole |
title_sort | determination of the bending field integral of the lep spectrometer dipole |
topic | Accelerators and Storage Rings |
url | https://dx.doi.org/10.1016/j.nima.2005.01.306 http://cds.cern.ch/record/799441 |
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