Measuring the intensity and position of a pA electron beam with resonant cavities

In order to continuously monitor the intensity and position of an electron beam of a few hundred pA, a system of resonant cavities has been set up. The current measurement relies on signals of a few fW power extracted out of a cylindrical resonator, excited at its TM_{010} mode. The demodulated cavi...

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Main Authors: Thorsten R. Pusch, F. Frommberger, W. C. A. Hillert, B. Neff
Format: Article
Language:English
Published: American Physical Society 2012-11-01
Series:Physical Review Special Topics. Accelerators and Beams
Online Access:http://doi.org/10.1103/PhysRevSTAB.15.112801
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spelling doaj-54b2fa0281f1422fa1b84da104a515342020-11-25T01:04:33ZengAmerican Physical SocietyPhysical Review Special Topics. Accelerators and Beams1098-44022012-11-01151111280110.1103/PhysRevSTAB.15.112801Measuring the intensity and position of a pA electron beam with resonant cavitiesThorsten R. PuschF. FrommbergerW. C. A. HillertB. NeffIn order to continuously monitor the intensity and position of an electron beam of a few hundred pA, a system of resonant cavities has been set up. The current measurement relies on signals of a few fW power extracted out of a cylindrical resonator, excited at its TM_{010} mode. The demodulated cavity pickup signal allows the reconstruction of the beam current with a precision of a few pA. For beam position measurements, we designed two resonators, one each for the horizontal and vertical plane. They are excited at their TM_{110} dipole modes, the signal strength vanishing with the beam passing on their symmetry axis. Commercial digital lock-in amplifiers perform a phase-sensitive detection of the position signals, separating them from background noise. A frequency mixing scheme was applied to transform the signals into the passband of the amplifiers. Great care was taken to prevent cross talk by using special shielding. With these techniques, a relative beam position resolution of 50  μm was achieved. The position readings are sampled with a maximum rate of 9 Hz. A standard PC is used to read out the lock-in amplifiers. It transfers the measured raw data as well as processed values to the accelerator control system for graphical display.http://doi.org/10.1103/PhysRevSTAB.15.112801
collection DOAJ
language English
format Article
sources DOAJ
author Thorsten R. Pusch
F. Frommberger
W. C. A. Hillert
B. Neff
spellingShingle Thorsten R. Pusch
F. Frommberger
W. C. A. Hillert
B. Neff
Measuring the intensity and position of a pA electron beam with resonant cavities
Physical Review Special Topics. Accelerators and Beams
author_facet Thorsten R. Pusch
F. Frommberger
W. C. A. Hillert
B. Neff
author_sort Thorsten R. Pusch
title Measuring the intensity and position of a pA electron beam with resonant cavities
title_short Measuring the intensity and position of a pA electron beam with resonant cavities
title_full Measuring the intensity and position of a pA electron beam with resonant cavities
title_fullStr Measuring the intensity and position of a pA electron beam with resonant cavities
title_full_unstemmed Measuring the intensity and position of a pA electron beam with resonant cavities
title_sort measuring the intensity and position of a pa electron beam with resonant cavities
publisher American Physical Society
series Physical Review Special Topics. Accelerators and Beams
issn 1098-4402
publishDate 2012-11-01
description In order to continuously monitor the intensity and position of an electron beam of a few hundred pA, a system of resonant cavities has been set up. The current measurement relies on signals of a few fW power extracted out of a cylindrical resonator, excited at its TM_{010} mode. The demodulated cavity pickup signal allows the reconstruction of the beam current with a precision of a few pA. For beam position measurements, we designed two resonators, one each for the horizontal and vertical plane. They are excited at their TM_{110} dipole modes, the signal strength vanishing with the beam passing on their symmetry axis. Commercial digital lock-in amplifiers perform a phase-sensitive detection of the position signals, separating them from background noise. A frequency mixing scheme was applied to transform the signals into the passband of the amplifiers. Great care was taken to prevent cross talk by using special shielding. With these techniques, a relative beam position resolution of 50  μm was achieved. The position readings are sampled with a maximum rate of 9 Hz. A standard PC is used to read out the lock-in amplifiers. It transfers the measured raw data as well as processed values to the accelerator control system for graphical display.
url http://doi.org/10.1103/PhysRevSTAB.15.112801
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