A simple method for determining dosimetric leaf gap with cross-field dose width for rounded leaf-end multileaf collimator systems

PurposeThe dosimetric leaf gap (DLG) and multileaf collimator (MLC) transmission are two important systematic parameters used to model the rounded MLC leaf ends effect when commissioning an Eclipse treatment planning system (TPS). Determining the optimal DLG is a time consuming process. This study develops a simple and reliable method for determining the DLG using the cross-field dose width.Methods and materialsA Varian TrueBeam linac with 6 MV, 10 MV, 6 MV flattening filter free (FFF) and 10 MV FFF photon beams and equipped with the 120 Millennium MLC and the Eclipse™ TPS was used in this study. Integral sliding fields and static slit MLC field doses with different gap widths were measured with an ionization chamber and GAFCHROMIC EBT3 films, respectively. Measurements were performed for different beam energies and at depths of 5 and 10 cm. DLGs were derived from a linear extrapolation to zero dose and intercepting at the gap width axis. In the ion chamber measurements method, the average MLC leaf transmission to the gap reading for each gap (RgT) were calculated with nominal and cross-field dose widths, respectively. The cross-field dose widths were determined according to the dose profile measured with EBT3 films. Additionally, the optimal DLG values were determined using plan dose measurements, as the value that produced the closest agreement between the planned and measured doses. DLGs derived from the nominal and cross-field dose width, the film measurements, and the optimal process, were obtained and compared.ResultsThe DLG values are insensitive to the variations in depth (within 0.07 mm). DLGs derived from nominal gap widths showed a significantly lower values (with difference about 0.5 mm) than that from cross-field dose widths and from film measurements and from plan optimal values. The method in deriving DLGs by correcting the nominal gap widths to the cross-field dose widths has shown good agreements to the plan optimal values (with difference within 0.21 mm).ConclusionsThe DLG values derived from the cross-field dose width method were consistent with the values derived from film measurements and from the plan optimal process. A simple and reliable method to determine DLG for rounded leaf-end MLC systems was established. This method provides a referable DLG value required during TPS commissioning.

[1]  Daniel A. Low,et al.  Basic Applications of Multileaf Collimators , 2001 .

[2]  Lei Wang,et al.  Verification of dosimetric accuracy on the TrueBeam STx: rounded leaf effect of the high definition MLC. , 2011, Medical physics.

[3]  Alejandra Rangel,et al.  Tolerances on MLC leaf position accuracy for IMRT delivery with a dynamic MLC. , 2009, Medical physics.

[4]  C. Ling,et al.  Physical and dosimetric aspects of a multileaf collimation system used in the dynamic mode for implementing intensity modulated radiotherapy. , 1998, Medical physics.

[5]  E Jiménez-Ortega,et al.  3D VMAT Verification Based on Monte Carlo Log File Simulation with Experimental Feedback from Film Dosimetry , 2016, PloS one.

[6]  Jinkoo Kim,et al.  IMRT and RapidArc commissioning of a TrueBeam linear accelerator using TG‐119 protocol cases , 2014, Journal of applied clinical medical physics.

[7]  D. Low,et al.  A technique for the quantitative evaluation of dose distributions. , 1998, Medical physics.

[8]  Tanya Kairn,et al.  Optimization of the dosimetric leaf gap for use in planning VMAT treatments of spine SABR cases , 2017, Journal of applied clinical medical physics.

[9]  Experimental characterization of the dosimetric leaf gap , 2016 .

[10]  Ravikumar Manickam,et al.  Comparison of four commercial devices for RapidArc and sliding window IMRT QA , 2011, Journal of applied clinical medical physics.

[11]  Santi Tofani,et al.  Dosimetric characterization and use of GAFCHROMIC EBT3 film for IMRT dose verification , 2013, Journal of applied clinical medical physics.

[12]  Hui Yan,et al.  Commissioning and dosimetric characteristics of TrueBeam system: composite data of three TrueBeam machines. , 2012, Medical physics.

[13]  Jinkoo Kim,et al.  Relationship between dosimetric leaf gap and dose calculation errors for high definition multi-leaf collimators in radiotherapy , 2018, Physics and imaging in radiation oncology.

[14]  K. Bush,et al.  Clinical significance of multi-leaf collimator positional errors for volumetric modulated arc therapy. , 2010, Radiotherapy and oncology : journal of the European Society for Therapeutic Radiology and Oncology.

[15]  I. Chetty,et al.  Precise film dosimetry for stereotactic radiosurgery and stereotactic body radiotherapy quality assurance using Gafchromic™ EBT3 films , 2016, Radiation Oncology.

[16]  Xiaowei Liu,et al.  The combination of the error correction methods of GAFCHROMIC EBT3 film , 2017, PloS one.

[17]  Stanislaw Szpala,et al.  On using the dosimetric leaf gap to model the rounded leaf ends in VMAT/RapidArc plans , 2014, Journal of applied clinical medical physics.

[18]  G T Chen,et al.  Intensity modulated radiotherapy dose delivery error from radiation field offset inaccuracy. , 2000, Medical physics.

[19]  Clive Baldock,et al.  An experimental investigation into the radiation field offset of a dynamic multileaf collimator , 2006, Physics in medicine and biology.

[20]  Jonathan G. Li,et al.  Comparison of two commercial detector arrays for IMRT quality assurance , 2009, Journal of Applied Clinical Medical Physics.

[21]  T Solberg,et al.  Commissioning of the Varian TrueBeam linear accelerator: a multi-institutional study. , 2013, Medical physics.

[22]  L Kumaraswamy,et al.  Spatial variation of dosimetric leaf gap and its impact on dose delivery. , 2014, Medical physics.