Dielectric-Filled Reentrant Cavity Resonator as a Low-Intensity Proton Beam Diagnostic

Measurement of the proton beam current (0.1–40 nA) at the medical treatment facility PROSCAN at the Paul Scherrer Institut (PSI) is performed with ionization chambers. To mitigate the scattering issues and to preserve the quality of the beam delivered to the patients, a non-interceptive monitor base...

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Main Authors: Sudharsan Srinivasan, Pierre-André Duperrex
Format: Article
Language:English
Published: MDPI AG 2018-11-01
Series:Instruments
Subjects:
Online Access:https://www.mdpi.com/2410-390X/2/4/24
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spelling doaj-ec8244126968478f87f711c48b5e1ac12020-11-25T00:37:13ZengMDPI AGInstruments2410-390X2018-11-01242410.3390/instruments2040024instruments2040024Dielectric-Filled Reentrant Cavity Resonator as a Low-Intensity Proton Beam DiagnosticSudharsan Srinivasan0Pierre-André Duperrex1Paul Scherrer Institut, Forschungsstrasse 111, PSI 5232 Villigen, SwitzerlandPaul Scherrer Institut, Forschungsstrasse 111, PSI 5232 Villigen, SwitzerlandMeasurement of the proton beam current (0.1–40 nA) at the medical treatment facility PROSCAN at the Paul Scherrer Institut (PSI) is performed with ionization chambers. To mitigate the scattering issues and to preserve the quality of the beam delivered to the patients, a non-interceptive monitor based on the principle of a reentrant cavity resonator has been built. The resonator with a fundamental resonance frequency of 145.7 MHz was matched to the second harmonic of the pulse repetition rate (72.85 MHz) of the beam extracted from the cyclotron. This was realized with the help of ANSYS HFSS (High Frequency Structural Simulator) for network analysis. Both, the pickup position and dielectric thickness were optimized. The prototype was characterized with a stand-alone test bench. There is good agreement between the simulated and measured parameters. The observed deviation in the resonance frequency is attributed to the frequency dependent dielectric loss tangent. Hence, the dielectric had to be resized to tune the resonator to the design resonance frequency. The measured sensitivity performances were in agreement with the expectations. We conclude that the dielectric reentrant cavity resonator is a promising candidate for measuring low proton beam currents in a non-destructive manner.https://www.mdpi.com/2410-390X/2/4/24beam diagnosticsANSYS HFSSnetwork analysisscattering parametersresonance frequencyQ factor
collection DOAJ
language English
format Article
sources DOAJ
author Sudharsan Srinivasan
Pierre-André Duperrex
spellingShingle Sudharsan Srinivasan
Pierre-André Duperrex
Dielectric-Filled Reentrant Cavity Resonator as a Low-Intensity Proton Beam Diagnostic
Instruments
beam diagnostics
ANSYS HFSS
network analysis
scattering parameters
resonance frequency
Q factor
author_facet Sudharsan Srinivasan
Pierre-André Duperrex
author_sort Sudharsan Srinivasan
title Dielectric-Filled Reentrant Cavity Resonator as a Low-Intensity Proton Beam Diagnostic
title_short Dielectric-Filled Reentrant Cavity Resonator as a Low-Intensity Proton Beam Diagnostic
title_full Dielectric-Filled Reentrant Cavity Resonator as a Low-Intensity Proton Beam Diagnostic
title_fullStr Dielectric-Filled Reentrant Cavity Resonator as a Low-Intensity Proton Beam Diagnostic
title_full_unstemmed Dielectric-Filled Reentrant Cavity Resonator as a Low-Intensity Proton Beam Diagnostic
title_sort dielectric-filled reentrant cavity resonator as a low-intensity proton beam diagnostic
publisher MDPI AG
series Instruments
issn 2410-390X
publishDate 2018-11-01
description Measurement of the proton beam current (0.1–40 nA) at the medical treatment facility PROSCAN at the Paul Scherrer Institut (PSI) is performed with ionization chambers. To mitigate the scattering issues and to preserve the quality of the beam delivered to the patients, a non-interceptive monitor based on the principle of a reentrant cavity resonator has been built. The resonator with a fundamental resonance frequency of 145.7 MHz was matched to the second harmonic of the pulse repetition rate (72.85 MHz) of the beam extracted from the cyclotron. This was realized with the help of ANSYS HFSS (High Frequency Structural Simulator) for network analysis. Both, the pickup position and dielectric thickness were optimized. The prototype was characterized with a stand-alone test bench. There is good agreement between the simulated and measured parameters. The observed deviation in the resonance frequency is attributed to the frequency dependent dielectric loss tangent. Hence, the dielectric had to be resized to tune the resonator to the design resonance frequency. The measured sensitivity performances were in agreement with the expectations. We conclude that the dielectric reentrant cavity resonator is a promising candidate for measuring low proton beam currents in a non-destructive manner.
topic beam diagnostics
ANSYS HFSS
network analysis
scattering parameters
resonance frequency
Q factor
url https://www.mdpi.com/2410-390X/2/4/24
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AT pierreandreduperrex dielectricfilledreentrantcavityresonatorasalowintensityprotonbeamdiagnostic
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