Purpose
At our institute, in vivo patient dose distributions are reconstructed for all treatments delivered using conventional linacs from electronic portal imaging device (EPID) transit images acquired during treatment using a simple backāprojection model. Currently, the clinical implementation of MRIāguided radiotherapy systems, which aims for online and realātime adaptation of the treatment plan, is progressing. In our department, the MRālinac (Unity, Elekta AB, Stockholm, Sweden) is now in clinical use. The aim of this work is to demonstrate the feasibility of twoādimensional (2D) EPID dosimetric verification for the magnetic resonance (MR)ālinac by comparing backāprojected EPID doses to ionization chamber (IC) array dose distributions.
Materials and methods
Our conventional backāprojection algorithm was adapted for the MRālinac. The most important changes involve modeling of the attenuation by and scatter from the cryostat. The commissioning process involved the acquisition of square field EPID measurements using various phantom setups (varying SSD, phantom thickness, and field size). Commissioning models were created for gantry 0Ā°, 90Ā°, and 180Ā° and verified by comparing EPIDāreconstructed 2D dose distributions to measurements made with the OCTAVIUS 1500 IC array (PTW, Freiburg, Germany) for two prostate and one rectum IMRT plans (25 beams total). The average of the Ī³ parameters (yāmean and yāpass rate) and the dose difference at a reference point were reported. Due to their construction, the attenuation of couch, bridge, and cryostat shows a much stronger dependence on gantry angle in the MRālinac compared to conventional linacs. We present a method to correct for these effects. This method is validated by dose reconstruction of the 25 intensityāmodulated radiation therapy beams recorded at a certain gantry angle using the model of another gantry angle, combined with the correction method.
Results
For dose verification performed at a gantry angle identical to the commissioned model, the average yāmean and yāpass rate values (3% global dose, 2Ā mm, 10% isodose) were 0.37Ā Ā±Ā 0.07 and 98.1, 95% CI [98.1Ā Ā±Ā 2.4], respectively. The average dose difference at the reference point was ā0.5%Ā Ā±Ā 1.8%. Verification at gantry angles different from the commissioned model (i.e., using the gantry angle dependent correction) reported 0.39Ā Ā±Ā 0.08 and 97.6, 95% CI [96.9, 98.3] average yāmean and yāpass rate values. The average dose difference at the reference point was ā0.1%Ā Ā±Ā 1.8%.
Conclusion
The EPID dosimetry backāprojection model was successfully adapted for the MRālinac at gantry 0Ā°, 90Ā°, and 180Ā°, accounting for the presence of the MRI housing between phantom (or patient) and the EPID. A method to account for the gantry angle dependence was also tested reporting similar results.