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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2012-11-01
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Series: | Physical Review Special Topics. Accelerators and Beams |
Online Access: | http://doi.org/10.1103/PhysRevSTAB.15.112801 |
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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 |
work_keys_str_mv |
AT thorstenrpusch measuringtheintensityandpositionofapaelectronbeamwithresonantcavities AT ffrommberger measuringtheintensityandpositionofapaelectronbeamwithresonantcavities AT wcahillert measuringtheintensityandpositionofapaelectronbeamwithresonantcavities AT bneff measuringtheintensityandpositionofapaelectronbeamwithresonantcavities |
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