Adjusting source modelling parameters for accurate dose calculations with the Oncentra Masterplan treatment planning system for small fields with dimensions of less than 5x5cm2

2014 ◽  
Vol 30 ◽  
pp. e76
Author(s):  
Malatar Georgia ◽  
S. Papatheodorou ◽  
V. Anastasis
2013 ◽  
Vol 55 ◽  
pp. 60-63 ◽  
Author(s):  
Jeong-Eun Rah ◽  
Dongho Shin ◽  
Jeong-hoon Park ◽  
Ui-Jung Hwang ◽  
Do Hoon Oh ◽  
...  

2015 ◽  
Vol 115 ◽  
pp. S413-S414
Author(s):  
F. Lobefalo ◽  
A. Fogliata ◽  
G. Reggiori ◽  
A. Stravato ◽  
L. Cozzi ◽  
...  

2019 ◽  
Vol 18 (4) ◽  
pp. 353-364
Author(s):  
Sepideh Behinaein ◽  
Ernest Osei ◽  
Johnson Darko ◽  
Paule Charland ◽  
Dylan Bassi

AbstractBackground:An increasing number of external beam treatment modalities including intensity modulated radiation therapy, volumetric modulated arc therapy (VMAT) and stereotactic radiosurgery uses very small fields for treatment planning and delivery. However, there are major challenges in small photon field dosimetry, due to the partial occlusion of the direct photon beam source’s view from the measurement point, lack of lateral charged particle equilibrium, steep dose-rate gradient and volume averaging effect of the detector response and variation of the energy fluence in the lateral direction of the beam. Therefore, experimental measurements of dosimetric parameters such as percent depth doses (PDDs), beam profiles and relative output factors (ROFs) for small fields continue to be a challenge.Materials and Methods:In this study, we used a homogeneous water phantom and the heterogeneous anthropomorphic stereotactic end-to-end verification (STEEV) head phantom for all dose measurements and calculations. PDDs, lateral dose profiles and ROFs were calculated in the Eclipse Treatment Planning System version 13·6 using the Acuros XB (AXB) and the analytical anisotropic algorithms (AAAs) in a homogenous water phantom. Monte Carlo (MC) simulations and measurements using the Exradin W1 Scintillator were also accomplished for four photon energies: 6 MV, 6FFF, 10 MV and 10FFF. Two VMAT treatment plans were generated for two different targets: one located in the brain and the other in the neck (close to the trachea) in the head phantom (CIRS, Norfolk, VA, USA). A Varian Truebeam linear accelerator (Varian, Palo Alto, CA, USA) was used for all treatment deliveries. Calculated results with AXB and AAA were compared with MC simulations and measurements.Results:The average difference of PDDs between W1 Exradin Scintillator measurements and MC simulations, AAA and AXB algorithm calculations were 1·2, 2·4 and 3·2%, respectively, for all field sizes and energies. AXB and AAA showed differences in ROF of about 0·3 and 2·9%, respectively, compared with W1 Exradin Scintillator measured values. For the target located in the brain in the head phantom, the average dose difference between W1 Exradin Scintillator and the MC simulations, AAA and AXB were 0·2, 3·2 and 2·7%, respectively, for all field sizes. Similarly, for the target located in the neck, the respective dose differences were 3·8, 5·7 and 3·5%.Conclusion:In this study, we compared dosimetric parameters such as PDD, beam profile and ROFs in water phantom and isocenter point dose measurements in an anthropomorphic head phantom representing a patient. We observed that measurements using the W1 Exradin scintillator agreed well with MC simulations and can be used efficiently for dosimetric parameters such as PDDs and dose profiles and patient-specific quality assurance measurements for small fields. In both homogenous and heterogeneous media, the AXB algorithm dose prediction agrees well with MC and measurements and was found to be superior to the AAA algorithm.


2001 ◽  
Vol 2 (2) ◽  
pp. 73-84 ◽  
Author(s):  
Christopher T. Baird ◽  
George Starkschall ◽  
H. Helen Liu ◽  
Thomas A. Buchholz ◽  
Kenneth R. Hogstrom

2018 ◽  
Vol 14 (7) ◽  
pp. 1110 ◽  
Author(s):  
Ashraf Farkhari ◽  
MohammadTaghi Bahreyni Toossi ◽  
Shokouhozaman Soleymanifard ◽  
Bagher Farhood ◽  
Courtney Knaup

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