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Synchrotrons for hadron therapy, part 1
The treatment of cancer with accelerator beams has a long history with linacs, cyclotrons and now synchrotrons being exploited for this purpose. Treatment techniques can be broadly divided into the use of spread-out beams and scanned 'pencil' beams. The Bragg-peak behaviour of hadrons make...
Autores principales: | , , , , , , , , |
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Lenguaje: | eng |
Publicado: |
1999
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1016/S0168-9002(99)00206-5 http://cds.cern.ch/record/379811 |
_version_ | 1780893364126744576 |
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author | Badano, L Benedikt, Michael Bryant, P J Crescenti, M Holy, P Knaus, P Maier, A T Pullia, M Rossi, S |
author_facet | Badano, L Benedikt, Michael Bryant, P J Crescenti, M Holy, P Knaus, P Maier, A T Pullia, M Rossi, S |
author_sort | Badano, L |
collection | CERN |
description | The treatment of cancer with accelerator beams has a long history with linacs, cyclotrons and now synchrotrons being exploited for this purpose. Treatment techniques can be broadly divided into the use of spread-out beams and scanned 'pencil' beams. The Bragg-peak behaviour of hadrons makes them ideal candidates for the latter. The combination of precisely focused 'pencil' beams with controllable penetration (Bragg peak) and high, radio-biological efficiency (light ions) opens the way to treating the more awkward tumours that are radio-resistant, complex in shape and lodged against critical organs. To accelerate light ions (probably carbon) with pulse-to-pulse energy variation, a synchrotron is the natural choice. The beam scanning system is controlled via an on-line measurement of the particle flux entering the patient and, for this reason, the beam spill must be extended in time (seconds) by a slow-extraction scheme. The quality of the dose intensity profile ultimately depends on the uniformity of the beam spill. This is the greatest challenge for the synchrotron, since slow-extraction schemes are notoriously sensitive. This paper reviews the extraction techniques, describes methods for smoothing the beam spill and outlines the implications for the extraction line and beam delivery system. |
id | cern-379811 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 1999 |
record_format | invenio |
spelling | cern-3798112021-11-11T09:54:17Zdoi:10.1016/S0168-9002(99)00206-5http://cds.cern.ch/record/379811engBadano, LBenedikt, MichaelBryant, P JCrescenti, MHoly, PKnaus, PMaier, A TPullia, MRossi, SSynchrotrons for hadron therapy, part 1Accelerators and Storage RingsThe treatment of cancer with accelerator beams has a long history with linacs, cyclotrons and now synchrotrons being exploited for this purpose. Treatment techniques can be broadly divided into the use of spread-out beams and scanned 'pencil' beams. The Bragg-peak behaviour of hadrons makes them ideal candidates for the latter. The combination of precisely focused 'pencil' beams with controllable penetration (Bragg peak) and high, radio-biological efficiency (light ions) opens the way to treating the more awkward tumours that are radio-resistant, complex in shape and lodged against critical organs. To accelerate light ions (probably carbon) with pulse-to-pulse energy variation, a synchrotron is the natural choice. The beam scanning system is controlled via an on-line measurement of the particle flux entering the patient and, for this reason, the beam spill must be extended in time (seconds) by a slow-extraction scheme. The quality of the dose intensity profile ultimately depends on the uniformity of the beam spill. This is the greatest challenge for the synchrotron, since slow-extraction schemes are notoriously sensitive. This paper reviews the extraction techniques, describes methods for smoothing the beam spill and outlines the implications for the extraction line and beam delivery system.CERN-PS-99-007-OPoai:cds.cern.ch:3798111999-01-29 |
spellingShingle | Accelerators and Storage Rings Badano, L Benedikt, Michael Bryant, P J Crescenti, M Holy, P Knaus, P Maier, A T Pullia, M Rossi, S Synchrotrons for hadron therapy, part 1 |
title | Synchrotrons for hadron therapy, part 1 |
title_full | Synchrotrons for hadron therapy, part 1 |
title_fullStr | Synchrotrons for hadron therapy, part 1 |
title_full_unstemmed | Synchrotrons for hadron therapy, part 1 |
title_short | Synchrotrons for hadron therapy, part 1 |
title_sort | synchrotrons for hadron therapy, part 1 |
topic | Accelerators and Storage Rings |
url | https://dx.doi.org/10.1016/S0168-9002(99)00206-5 http://cds.cern.ch/record/379811 |
work_keys_str_mv | AT badanol synchrotronsforhadrontherapypart1 AT benediktmichael synchrotronsforhadrontherapypart1 AT bryantpj synchrotronsforhadrontherapypart1 AT crescentim synchrotronsforhadrontherapypart1 AT holyp synchrotronsforhadrontherapypart1 AT knausp synchrotronsforhadrontherapypart1 AT maierat synchrotronsforhadrontherapypart1 AT pulliam synchrotronsforhadrontherapypart1 AT rossis synchrotronsforhadrontherapypart1 |