SU-E-T-731: The Effect of Thermoplatic Mask to the Surface Dose in Sterotactic Brain Treatments with Flattening Filter Free Beams with EBT3 Gafchromic Film and OSL Dosimeter

2015 ◽  
Vol 42 (6Part24) ◽  
pp. 3505-3505
Author(s):  
G Yilidir ◽  
H Acar ◽  
N Kucuk ◽  
E Kucukmorkoc ◽  
M Doyuran ◽  
...  
2015 ◽  
Vol 42 (6Part23) ◽  
pp. 3502-3502
Author(s):  
M Meshram ◽  
S Pramanik ◽  
C P Ranjith ◽  
M Meshram

2013 ◽  
Vol 40 (6Part11) ◽  
pp. 225-225
Author(s):  
Darrell TH Li ◽  
Michael LM Cheung ◽  
Louis KY Lee ◽  
Michael KM Kam ◽  
Brian KH Yu ◽  
...  

Author(s):  
Gopinath Mamballikalam ◽  
S Senthilkumar ◽  
P. M. Jayadevan ◽  
R. C. Jaon bos ◽  
P. M. Ahamed Basith ◽  
...  

Abstract Purpose: This study aims to evaluate dosimetric parameters like percentage depth dose, dosimetric field size, depth of maximum dose surface dose, penumbra and output factors measured using IBA CC01 pinpoint chamber, IBA stereotactic field diode (SFD), PTW microDiamond against Monte Carlo (MC) simulation for 6 MV flattening filter-free small fields. Materials and Methods: The linear accelerator used in the study was a Varian TrueBeam® STx. All field sizes were defined by jaws. The required shift to effective point of measurement was given for CC01, SFD and microdiamond for depth dose measurements. The output factor of a given field size was taken as the ratio of meter readings normalised to 10 × 10 cm2 reference field size without applying any correction to account for changes in detector response. MC simulation was performed using PRIMO (PENELOPE-based program). The phase space files for MC simulation were adopted from the MyVarian Website. Results and Discussion: Variations were seen between the detectors and MC, especially for fields smaller than 2 × 2 cm2 where the lateral charge particle equilibrium was not satisfied. Diamond detector was seen as most suitable for all measurements above 1 × 1 cm2. SFD was seen very close to MC results except for under-response in output factor measurements. CC01 was observed to be suitable for field sizes above 2 × 2 cm2. Volume averaging effect for penumbra measurements in CC01 was observed. No detector was found suitable for surface dose measurement as surface ionisation was different from surface dose due to the effect of perturbation of fluence. Some discrepancies in measurements and MC values were observed which may suggest effects of source occlusion, shift in focal point or mismatch between real accelerator geometry and simulation geometry. Conclusion: For output factor measurement, TRS483 suggested correction factor needs to be applied to account for the difference in detector response. CC01 can be used for field sizes above 2 × 2 cm2 and microdiamond detector is suitable for above 1 × 1 cm2. Below these field sizes, perturbation corrections and volume averaging corrections need to be applied.


2020 ◽  
Vol 188 (3) ◽  
pp. 285-298
Author(s):  
Trinitat García-Hernández ◽  
Aurora Vicedo-González ◽  
Beatriz Sánchez-Nieto ◽  
Maite Romero-Expósito ◽  
Joan Roselló-Ferrando

Abstract There is a growing interest in the use of flattening filter free (FFF) beams due to the shorter treatment times. The reduction of head scatter suggests a better radiation protection to radiotherapy patients, considering the expected decrease in peripheral surface dose (PSD). In this work, PSD of flattened (FF) and FFF-photon beams was compared. A radiochromic film calibration method to reduce energy dependence was used. PSD was measured at distances from 2 to 50 cm to the field border for different square field sizes, modifying relevant clinical parameters. Also, clinical breast and prostate stereotactic body radiotherapy (SBRT) plans were studied. For square beams, FFF PSD is lower compared with FF PSD (differences ranging from 3 to 64%) and 10 MV FFF yields to the lowest value, for distances greater than 5 cm. For SBRT plans, near and far away from the field border, there is a reduction of PSD for FFF-beams, but the behavior at intermediate distances should be checked depending on the case.


2012 ◽  
Vol 83 (2) ◽  
pp. e281-e285 ◽  
Author(s):  
Yuenan Wang ◽  
Mohammad K. Khan ◽  
Joseph Y. Ting ◽  
Stephen B. Easterling

2019 ◽  
Vol 4 (4) ◽  
pp. 571-578 ◽  
Author(s):  
Andrew R. Barsky ◽  
Fionnbarr O'Grady ◽  
Christopher Kennedy ◽  
Neil K. Taunk ◽  
Lei Dong ◽  
...  

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