Search

Purpose To perform a three-dimensional (3D) concurrent isocentricity measurement of a clinical linear accelerator's (linac) using a single 3D dosimeter, PRESAGE. Methods A 3D dosimeter, PRESAGE, set up on the treatment couch of a Varian TrueBeam LINAC using the setup lasers, was irradiated under gantry angles of 0 ∘ , 50 ∘ , 160 ∘ , and 270 ∘ with the couch fixed at 0 ∘ and subsequently, under couch angles of 10 ∘ , 330 ∘ , 300 ∘ , and 265 ∘ with the gantry fixed at 270 ∘ . The 1 cm 2 (at 100 cm SAD) square fields were delivered at 6 MV with 800 MU/field. After irradiation, the dosimeter was scanned using a single-beam optical scanner and images were reconstructed with submillimeter resolution using filtered back-projection. Postprocessing was used to extract views parallel to the star-shot planes from which beam trajectories and the smallest circles enclosing these were drawn and extracted. These circles and information from the view orthogonal to both star-shots were used to represent the rotational centers as spheroids. The linac isocenter was defined by the distribution of midpoints between any, randomly selected, points lying inside the center spheroids defined by the table and gantry rotations; isocenter location and size were defined by the average midpoint and the distribution's semi-axes. Collimator rotations were not included in this study. Results Relative to the setup center defined by lasers, the table and gantry rotation center coordinates (lat., long., vert.) were measured in units of millimeters, to be (-0.24, 0.18, -0.52) and (0.10, 0.53, -0.52), respectively. Displacements from the setup center were 0.60 and 0.75 mm for the table and gantry centers, while the distance between them measured 0.49 mm. The linac's radiation isocenter was calculated to be at (-0.07, -0.17, 0.51) relative to the setup lasers and its size was found to be most easily described by a spheroid prolate in vertical direction with semi-axis lengths of 0.13 and 0.23 mm for the lateral-longitudinal and vertical directions, respectively. Conclusions This study demonstrates how to measure the location and sizes of rotational centers in 3D with one setup. The proposed method provides a more comprehensive view on the isocentricity of LINAC than the conventional two-dimensional film measurements. Additionally, a new definition of isocenter and its size was proposed.

Purpose Cherenkov light emission has been shown to correlate with ionizing radiation dose delivery in solid tissue. An important clinical application of Cherenkov light is the real-time verification of radiation treatment delivery in vivo. To test the feasibility of treatment field verification, Cherenkov light images were acquired concurrent with radiation beam delivery to standard and anthropomorphic phantoms. Specifically, we tested two clinical treatment scenarios: (a) Observation of field overlaps or gaps in matched 3D fields and (b) Patient positioning shifts during intensity modulated radiation therapy (IMRT) field delivery. Further development of this technique would allow real-time detection of treatment delivery errors on the order of millimeters so that patient safety and treatment quality can be improved. Methods Cherenkov light emission was captured using a PI-MAX4 intensified charge coupled device (ICCD) system (Princeton Instruments). All radiation delivery was performed using a Varian Trilogy linear accelerator (linac) operated at 6 MV or 18 MV for photon and 6 MeV or 16 MeV for electron studies. Field matching studies were conducted with photon and electron beams at gantry angles of 0°, 15°, and 45°. For each modality and gantry angle, a total of three data sets were acquired. Overlap and gap distances of 0, 2, 5, and 10 mm were tested and delivered to solid phantom material of 30 × 30 × 5 cm3 . Phantom materials used were white plastic water and brown solid water. Tests were additionally performed on an anthropomorphic phantom with an irregular surface. Positioning shift studies were performed using IMRT fields delivered to a thoracic anthropomorphic phantom. For thoracic phantom measurements, the camera was placed laterally to observe the entire right side of the phantom. Fields were delivered with known translational patient positioning shifts in four directions. Changes in the Cherenkov fluence were evaluated through the generation of difference maps from unshifted Cherenkov images. All images were evaluated using ImageJ, Python, and MATLAB software packages. Results For matched fields, Cherenkov images were able to quantitate matched field separations with discrepancies between 2 and 4 mm, depending on gantry angle and beam energy or modality. For all photon and electron beams delivered at a gantry angle of 0°, image analysis indicated average discrepancies of less than 2 mm for all field gaps and overlaps, with 83% of matched fields exhibiting discrepancies less than 1 mm. Beams delivered obliquely to the phantom surface exhibited average discrepancies as high as 4 mm for electron beams delivered at large oblique angles. Finally, for IMRT field delivery, vertical and lateral patient positioning shifts of 2 mm were detected in some cases, indicating the potential detectability threshold of using this technique alone. Conclusions Our study indicates that Cherenkov imaging can be used to support and bolster current treatment delivery verification techniques, improving our ability to recognize and rectify millimeter-scale delivery and positioning errors.

Purpose The precise dosimetric and geometric characteristics of small animal irradiators are essential to achieving reproducible dose delivery, especially in cases where image-guidance is utilized. Currently, radiochromic film is the established measurement tool used to evaluate beam characteristics for these systems. However, only 2D information can be acquired with film. This study characterized both the dosimetric and geometric properties of the small animal research radiation platform (SARRP, Xstrahl) for commissioning purposes using a 3D radiochromic dosimetry system with a submillimeter resolution optical computed tomography (OCT) scanner. Methods Like a modern clinical linear accelerator, the SARRP features both a beam delivery system and a cone beam computed tomography (CBCT) imaging system. Dosimetric and geometric characteristics of the SARRP were studied using EBT3 radiochromic film and 3D PRESAGE dosimeters. Dosimetric measurements included percent depth dose (PDD) curves and beam profiles. For geometric evaluation, the isocenter sizes of the treatment stage and gantry rotations as well as their coincidence were measured using star shot patterns. A commercial Epson Expression 11000XL flatbed scanner was used for readout of irradiated EBT3 films at 300 dpi resolution. Each irradiated PRESAGE dosimeter was scanned using a submillimeter resolution single laser beam OCT scanner. Acquired data were reconstructed with a resolution of 0.3 mm/pixel. Results PDD data measured from films and 3D dosimeters agree to within ±3% for depths up to 5 cm, for both 3 × 3 and 10 × 10 mm2 fixed collimation. Profiles were analyzed at 10, 20, and 30 mm depth for 3 × 3 mm2 and 10 × 10 mm2 fields. The FWHM measurements for both dosimeters agreed to within 0.01 mm, and the penumbras agreed to within 0.1 mm for 3 × 3 mm2 and 0.5 mm for 10 × 10 mm2 . Gantry and treatment stage isocenter sizes were determined to be 0.21 and 0.43 mm using EBT3 film, and 1.72 and 0.75 mm using PRESAGE dosimeters. Absolute isocenter shifts, evaluated with 3D phantoms, were 0.80 mm for the gantry rotation isocenter (treatment isocenter) with respect to the laser-defined setup isocenter, and 0.71 mm for the gantry rotation isocenter relative to treatment stage rotation isocenter (CBCT isocenter). The difference between CBCT isocenter and laser-defined setup isocenter was 0.68 mm. Conclusions This study demonstrated that 3D PRESAGE dosimeters can be used for verification of precise targeting for the SARRP. This 3D dosimetry system can be utilized to obtain information on both geometric and dosimetric properties, as well as acquire beam data parameters for the purpose of commissioning image-guided small animal irradiator systems.