Fast 2D phantom dosimetry for scanning proton beams

被引:108
作者
Boon, SN
van Luijk, P
Schippers, JM
Meertens, H
Denis, JM
Vynckier, S
Medin, J
Grusell, E
机构
[1] Kernfys Versneller Inst, NL-9747 AA Groningen, Netherlands
[2] Acad Ziekenhuis, Afdeling Radiotherapie, NL-9700 RB Groningen, Netherlands
[3] Univ Catholique Louvain, Clin Univ St Luc, Dept Radiotherapy & Oncol, B-1200 Brussels, Belgium
[4] Univ Uppsala, Dept Oncol, S-75121 Uppsala, Sweden
关键词
proton dosimetry; scintillators; scanning beams; dynamic treatments; intensity modulation; quality control;
D O I
10.1118/1.598221
中图分类号
R8 [特种医学]; R445 [影像诊断学];
学科分类号
1002 ; 100207 ; 1009 ;
摘要
A quality control system especially designed for dosimetry in scanning proton beams has been designed and tested. The system consists of a scintillating screen (Gd2O2S:Tb), mounted at the beam-exit side of a phantom, and observed by a low noise CCD camera with a long integration time. The purpose of the instrument is to make a fast and accurate two-dimensional image of the dose distribution at the screen position in the phantom. The linearity of the signal with the dose, the noise in the signal, the influence of the ionization density on the signal, and the influence of the field size on the signal have been investigated. The spatial resolution is 1.3 mm (1 s.d.), which is sufficiently smaller than typical penumbras in dose distributions, The measured yield depends linearly on the dose and agrees within 5% with the calculations. In the images a signal to noise ration (signal/l s.d.) of 10(2) has been found, which is in the same order of magnitude as expected from the calculations. At locations in the dose distribution possessing a strong contribution of high ionization densities (i.e., in the Bragg peak), we found some quenching of the light output, which can be described well by existing models if the beam characteristics are known. For clinically used beam characteristics such as a Spread Out Bragg peak, there is at most 8% deviation from the NACP ionization chamber measurements. The conclusion is that this instrument is a useful tool for quick and reliable quality control of proton beams. The long integration-time capabilities of the system make it worthwhile to investigate its applicability in scanning proton beams and other dynamic treatment modalities. (C) 1998 American Association of Physicists in Medicine. [S0094-2405(98)02104-X].
引用
收藏
页码:464 / 475
页数:12
相关论文
共 41 条
[1]   Physical characteristics of a commercial electronic portal imaging device [J].
Althof, VGM ;
deBoer, JCJ ;
Huizenga, H ;
Stroom, JC ;
Visser, AG ;
Swanenburg, BN .
MEDICAL PHYSICS, 1996, 23 (11) :1845-1855
[2]  
[Anonymous], 1967, THEORY PRACTICE SCIN
[3]   LIGHT OUTPUT AND ENERGY RESOLUTION OF CSI, YAG, GSO, BGO AND LSO SCINTILLATORS FOR LIGHT-IONS [J].
AVDEICHIKOV, VV ;
BERGHOLT, L ;
GUTTORMSEN, M ;
TAYLOR, JE ;
WESTERBERG, L ;
JAKOBSSON, B ;
KLAMRA, W ;
MURIN, YA .
NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION A-ACCELERATORS SPECTROMETERS DETECTORS AND ASSOCIATED EQUIPMENT, 1994, 349 (01) :216-224
[4]   NON-LINEAR RESPONSE OF PLASTIC SCINTILLATOR NE102 [J].
BADHWAR, GD ;
DENEY, CL ;
DENNIS, BR ;
KAPLON, MF .
NUCLEAR INSTRUMENTS & METHODS, 1967, 57 (01) :116-&
[5]  
BETHE HA, 1953, EXPT NUCL PHYSICS, V1, P200
[6]   Two-dimensional exit dosimetry using a liquid-filled electronic portal imaging device and a convolution model [J].
Boellaard, R ;
vanHerk, M ;
Uiterwaal, H ;
Mijnheer, B .
RADIOTHERAPY AND ONCOLOGY, 1997, 44 (02) :149-157
[7]   A REVIEW OF ELECTRONIC PORTAL IMAGING DEVICES (EPIDS) [J].
BOYER, AL ;
ANTONUK, L ;
FENSTER, A ;
VANHERK, M ;
MEERTENS, H ;
MUNRO, P ;
REINSTEIN, LE ;
WONG, J .
MEDICAL PHYSICS, 1992, 19 (01) :1-16
[8]  
BUCHANAN R, 1972, IEEE T NUCL SCI, V19, P3
[9]   INSTRUMENTATION FOR TREATMENT OF CANCER USING PROTON AND LIGHT-ION BEAMS [J].
CHU, WT ;
LUDEWIGT, BA ;
RENNER, TR .
REVIEW OF SCIENTIFIC INSTRUMENTS, 1993, 64 (08) :2055-2122
[10]   ANALYSIS OF RESPONSE DATA FOR SEVERAL ORGANIC SCINTILLATORS [J].
CRAUN, RL ;
SMITH, DL .
NUCLEAR INSTRUMENTS & METHODS, 1970, 80 (02) :239-&