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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...

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Autores principales: Chritin, R, Cornuet, D, Dehning, Bernd, Hidalgo, A, Hildreth, M, Kalbreier, Willi, Leclère, P, Mugnai, G, Palacios, J, Roncarolo, F, Torrence, E, Wilkinson, G
Lenguaje:eng
Publicado: 2004
Materias:
Acceso en línea:https://dx.doi.org/10.1016/j.nima.2005.01.306
http://cds.cern.ch/record/799441
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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.
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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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