The characterization of unflattened photon beams from a 6 MV linear accelerator

Commissioning data have been measured for an Elekta Precise linear accelerator running at 6 MV without a flattening filter with the aim of studying the effects of flattening filter removal on machine operation and beam characterization. Modern radiotherapy practice now routinely relies on the use of fluence modifying techniques such as IMRT, i.e. the active production of non-flat beams. For these techniques the flattening filter should not be necessary. It is also possible that the increased intensity around the central axis associated with unflattened beams may be useful for conventional treatment planning by acting as a field-in-field or integrated boost technique. For this reason open and wedged field data are presented. Whilst problems exist in running the machine filter free clinically, this paper shows that in many ways the beam is actually more stable, exhibiting almost half the variation in field symmetry for changes in steering and bending currents. Dosimetric benefits are reported here which include a reduction in head scatter by approx. 70%, decreased penumbra (0.5 mm), lower dose outside of the field edge (11%) and a doubling in dose rate (2.3 times for open and 1.9 times for wedged fields). Measurements also show that reduced scatter also reduces leakage radiation by approx. 60%, significantly lowering whole body doses. The greatest benefit of filter-free use is perceived to be for IMRT where increased dose rate combined with reduced head scatter and leakage radiation should lead to improved dose calculation, giving simpler, faster and more accurate dose delivery with reduced dose to normal tissues.

[1]  M T Gillin,et al.  Measurements of in-air output ratios for a linear accelerator with and without the flattening filter. , 2006, Medical physics.

[2]  U Titt,et al.  A flattening filter free photon treatment concept evaluation with Monte Carlo. , 2006, Medical physics.

[3]  U Titt,et al.  Monte Carlo study of backscatter in a flattening filter free clinical accelerator. , 2006, Medical physics.

[4]  K L Lam,et al.  Flattening-filter-based empirical methods to parametrize the head scatter factor. , 1996, Medical physics.

[5]  B. Nilsson Electron contamination from different materials in high energy photon beams. , 1985, Physics in medicine and biology.

[6]  M. Cohen Central axis depth dose data for use in radiotherapy. General introduction. , 1972, The British journal of radiology.

[7]  A L Boyer,et al.  Modeling the extrafocal radiation and monitor chamber backscatter for photon beam dose calculation. , 2001, Medical physics.

[8]  Asghar Mesbahi,et al.  Dosimetric characteristics of unflattened 6 MV photon beams of a clinical linear accelerator: a Monte Carlo study. , 2007, Applied radiation and isotopes : including data, instrumentation and methods for use in agriculture, industry and medicine.

[9]  Timothy C Zhu,et al.  Head scatter off-axis for megavoltage x rays. , 2003, Medical physics.

[10]  Eric E. Klein,et al.  Surface and buildup dose characteristics for 6, 10, and 18 MV photons from an Elekta Precise linear accelerator , 2003, Journal of applied clinical medical physics.

[11]  G Bruggmoser,et al.  Determination of the recombination correction factor kS for some specific plane-parallel and cylindrical ionization chambers in pulsed photon and electron beams , 2007, Physics in medicine and biology.

[12]  M. Roos,et al.  Measurement of saturation correction factors of thimble-type ionization chambers in pulsed photon beams , 1993 .

[13]  T C Zhu,et al.  The fraction of photons undergoing head scatter in x-ray beams. , 1995, Physics in medicine and biology.

[14]  J M Wilkinson,et al.  Electron contamination and build-up doses in conformal radiotherapy fields. , 1999, Physics in medicine and biology.

[15]  Radhe Mohan,et al.  Properties of unflattened photon beams shaped by a multileaf collimator. , 2006, Medical physics.

[16]  Radhe Mohan,et al.  Dosimetric properties of photon beams from a flattening filter free clinical accelerator , 2005, Physics in medicine and biology.

[17]  Radhe Mohan,et al.  Monte Carlo study of photon fields from a flattening filter-free clinical accelerator. , 2006, Medical physics.

[18]  Murray Boles,et al.  Central axis depth dose data for use in radiotherapy. A survey of depth doses and related data measured in water or equivalent media. , 1972, British journal of radiology. Supplement.

[19]  D Yan,et al.  Monitor unit settings for intensity modulated beams delivered using a step-and-shoot approach. , 2000, Medical physics.

[20]  Jianrong Dai,et al.  Delivery time comparison for intensity-modulated radiation therapy with/without flattening filter: a planning study. , 2004, Physics in medicine and biology.

[21]  R Mohan,et al.  Investigation of buildup dose from electron contamination of clinical photon beams. , 1983, Medical physics.

[22]  J M Wilkinson,et al.  Head scatter modelling for irregular field shaping and beam intensity modulation. , 1997, Physics in medicine and biology.

[23]  M. Alber,et al.  A virtual photon source model of an Elekta linear accelerator with integrated mini MLC for Monte Carlo based IMRT dose calculation , 2007, Physics in medicine and biology.

[24]  Y. Krutman,et al.  On the existence of low-energy photons (<150 keV) in the unflattened x-ray beam from an ordinary radiotherapeutic target in a medical linear accelerator , 2005, Physics in medicine and biology.