MR-Guided Radiation Therapy (MRIgRT) has been made possible only due to the ingenuity and commitment of commercial radiation therapy system vendors. Unlike conventional linear accelerator systems, MRIgRT systems have had to overcome significant and previously untested techniques to integrate the MRI systems with the radiation therapy delivery systems. Each of these three commercial systems has developed different approaches to integrating their MR and Linac functions. Each has also decided on a different main magnetic field strength, from 0.35T to 1.5T, as well as different design philosophies for other systems, such as the patient support assembly and treatment planning workflow. This paper is intended to provide the reader with a detailed understanding of each system's configuration so that the reader can better interpret the scientific literature concerning these commercial MRIgRT systems.
Section snippetsIntroduction to the 0.35T SystemThe first generation 0.35T system began as a Cobalt-driven radiation therapy machine (FDA cleared in 2012 with first patient treated in 2014).1,2 To accelerate the clinical application of MRgRT, the manufacturer used 3 Cobalt heads producing a total of 600 cGy per minute total at isocenter with fresh sources rather than await the MR-Linac development. In 2016 (FDA cleared in 2017), the manufacturer successfully modified their MRgRT system to utilize a linear accelerator, leading to the
Introduction to the 0.5T SystemThe rotating open bi-planar linac-MR system (Alberta LMR) was developed since 2005 and has installed at the Cross Cancer Institute (CCI) and University of Alberta (UofA), Edmonton, Alberta, Canada and shown in (Fig. 4). It has been commercialized in Edmonton. The system was designed from the ground up to specifically provide MR-guidance without compromising the advantages of current image guided radiotherapy practices. The open bi-planar design allows the option of placing the radiation beam
Extensive Couch Positioning for Planned or Offset TargetsOn the LMR the Kevlar couch has a longitudinal length of 260 cm. There are three translational degrees of freedom with maximum vertical speed of 5 cm/s and maximum horizontal speeds of 15 cm/s. It offers vertical and lateral ± 23 cm which makes it unique in this sector. This allows the positioning of any target, including targets that are strongly offset, at the planned position or at the isocenter. 3D target positioning is performed when these couch motions are used in tandem with the
Introduction to the 1.5T SystemThis section presents a brief overview of the development of the 1.5T MRIgRT system, a radiotherapy system with integrated 1.5T MRI functionality for high precision targeting (Fig. 5). The clinical potential and its applications are beyond the scope of this work, Hall et al.24 is one of the starting points for the clinical work related to the 1.5T system.
References (58)G Li et al.Artificial intelligence in radiotherapySemin Cancer Biol
(2022)
TN van de Lindt et al.Retrospective self-sorted 4D-MRI for the liverRadiother Oncol
(2018)
P Uijtewaal et al.First experimental demonstration of VMAT combined with MLC tracking for single and multi fraction lung SBRT on an MR-linacRadiother Oncol
(2022)
R Westley et al.HERMES: Delivery of a speedy prostate cancer treatmentClin Oncol (R Coll Radiol)
(2022)
B Cai et al.Performance of a multi leaf collimator system for MR-guided radiation therapyMed Phys
(2017)
C Kirkby et al.Lung dosimetry in a linac-MRI radiotherapy unit with a longitudinal magnetic fieldMed Phys
(2010)
R Yang et al.A novel transport sweep architecture for efficient deterministic patient dose calculations in MRI-guided radiotherapyPhys Med Biol
(2019)
R Yang et al.Feasibility of energy adaptive angular meshing for perpendicular and parallel magnetic fields in a grid based Boltzmann solverBiomed Phys Eng Express
(2020)
M Reynolds et al.Dose response of selected ion chambers in applied homogeneous transverse and longitudinal magnetic fieldsMed Phys
(2013)
M Reynolds et al.Dose response of selected solid state detectors in applied homogeneous transverse and longitudinal magnetic fieldsMed Phys
(2014)
M Reynolds et al.Technical note: Response measurement for select radiation detectors in magnetic fieldsMed Phys
(2015)
M Reynolds et al.Technical note: Ion chamber angular dependence in a magnetic fieldMed Phys
(2017)
M Reynolds et al.Technical note: Sensitive volume effects on ion chamber responses in longitudinal magnetic fieldsMed Phys
(2019)
VN Malkov et al.Sensitive volume effects on Monte Carlo calculated ion chamber response in magnetic fieldsMed Phys
(2017)
J Yun et al.First demonstration of intrafractional tumor-tracked irradiation using 2D phantom MR images on a prototype Linac-MRMed Phys
(2013)
J Yun et al.An artificial neural network (ANN)-based lung-tumor motion predictor for intrafractional MR tumor trackingMed Phys
(2012)
J Yun et al.Evaluation of a lung tumor autocontouring algorithm for intrafractional tumor tracking using low-field MRI: A phantom studyMed Phys
(2012)
E Yip et al.SU-E-J-151: Evaluation of a real time tumour autocontouring algorithm using in-vivo lung MR images with various contrast to noise ratiosMed Phys
(2012)
N Tahmasebi et al.Real-time lung tumor tracking using a CUDA enabled nonrigid registration algorithm for MRIIEEE J Transl Eng Health Med
(2020)
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