Synchrotrons for hadron therapy: Part I

被引:21
作者
Badano, L
Benedikt, M
Bryant, P
Crescenti, M
Holy, P
Knaus, P
Maier, A
Pullia, M
Rossi, S
机构
[1] TERA Fdn, I-28100 Novara, Italy
[2] CERN, DS Div, CH-1211 Geneva 23, Switzerland
[3] Med AUSTRON, A-2700 Wr Neustadt, Austria
[4] Oncol 2000 Fdn, CZ-12808 Prague 2, Czech Republic
关键词
synchrotron; slow extraction; hadron therapy;
D O I
10.1016/S0168-9002(99)00206-5
中图分类号
TH7 [仪器、仪表];
学科分类号
0804 ; 080401 ; 081102 ;
摘要
The treatment of cancer with accelerator beams has a long history with betatrons, 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 (C) 1999 Elsevier Science B.V. All rights reserved.
引用
收藏
页码:512 / 522
页数:11
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