A non-axial superconducting magnet design for optimized patient access and minimal SAD for use in a Linac-MR hybrid: proof of concept

A prototype rotating hybrid magnetic resonance imaging system and linac has been developed to allow for simultaneous imaging and radiation delivery parallel to B 0. However, the design of a compact magnet capable of rotation in a small vault with sufficient patient access and a typical clinical source-to-axis distance (SAD) is challenging. This work presents a novel superconducting magnet design as a proof of concept that allows for a reduced SAD and ample patient access by moving the superconducting coils to the side of the yoke. The yoke and pole-plate structures are shaped to direct the magnetic flux appropriately. The outer surface of the pole plate is optimized subject to the minimization of a cost function, which evaluates the uniformity of the magnetic field over an ellipsoid. The magnetic field calculations required in this work are performed with the 3D finite element method software package Opera-3D. Each tentative design strategy is virtually modeled in this software package, which is externally controlled by MATLAB, with its key geometries defined as variables. The optimization variables are the thickness of the pole plate at control points distributed over the pole plate surface. A novel design concept as a superconducting non-axial magnet is introduced, which could create a large uniform B 0 magnetic field with fewer geometric restriction. This non-axial 0.5 T superconducting magnet has a moderately reduced SAD of 123 cm and a vertical patient opening of 68 cm. This work is presented as a proof of principle to investigate the feasibility of a non-axial magnet with the coils located around the yoke, and the results encourage future design optimizations to maximize the benefits of this non-axial design.

[1]  T. Hiratani,et al.  Magnetic properties and workability of 6.5% Si steel sheet , 1996 .

[2]  J. Nagamatsu,et al.  Superconductivity at 39 K in Magnesium Diboride. , 2001 .

[3]  B Gino Fallone,et al.  Characterization, prediction, and correction of geometric distortion in 3 T MR images. , 2007, Medical physics.

[4]  Vadim Kuperman,et al.  Magnetic Resonance Imaging: Physical Principles and Applications , 2000 .

[5]  B G Fallone,et al.  Lung dosimetry in a linac-MRI radiotherapy unit with a longitudinal magnetic field. , 2010, Medical physics.

[6]  R. Marabotto,et al.  Construction and Operation of Cryogen Free ${\hbox{MgB}}_{2}$ Magnets for Open MRI Systems , 2008, IEEE Transactions on Applied Superconductivity.

[7]  D. Raabe,et al.  Overview of Microstructure and Microtexture Development in Grain-oriented Silicon Steel , 2006 .

[8]  K Wachowicz,et al.  Minimal skin dose increase in longitudinal rotating biplanar linac-MR systems: examination of radiation energy and flattening filter design. , 2016, Physics in medicine and biology.

[9]  J. Simkin,et al.  On the use of the total scalar potential on the numerical solution of fields problems in electromagnetics , 1979 .

[10]  Mark Holden,et al.  Detection and correction of geometric distortion in 3D MR images , 2001, SPIE Medical Imaging.

[11]  Riccardo Poli,et al.  Particle swarm optimization , 1995, Swarm Intelligence.

[12]  Deming Wang,et al.  A novel phantom and method for comprehensive 3-dimensional measurement and correction of geometric distortion in magnetic resonance imaging. , 2004, Magnetic resonance imaging.

[13]  Stuart Crozier,et al.  The Australian magnetic resonance imaging-linac program. , 2014, Seminars in radiation oncology.

[14]  J G M Kok,et al.  Integrating a 1.5 T MRI scanner with a 6 MV accelerator: proof of concept , 2009, Physics in medicine and biology.

[15]  João M.A. Rebello,et al.  Development of a magnetic sensor for detection and sizing of internal pipeline corrosion defects , 2009 .

[16]  Martin O Leach,et al.  A complete distortion correction for MR images: I. Gradient warp correction , 2005, Physics in medicine and biology.

[17]  B. Fallone,et al.  The rotating biplanar linac-magnetic resonance imaging system. , 2014, Seminars in radiation oncology.

[18]  A. J. Davies,et al.  On the use of the total scalar potential in the numerical solution of field problems in electromagnetics , 1988 .

[19]  J. Simkin,et al.  Three Dimensional non-linear electromagnetic field computation using scalar potentials , 1980 .

[20]  B. Fallone,et al.  First MR images obtained during megavoltage photon irradiation from a prototype integrated linac-MR system. , 2009, Medical physics.

[21]  M. Sumption,et al.  Microstructures and superconducting properties of high performance MgB2 thin films deposited from a high-purity, dense Mg-B target. , 2015, Applied surface science.

[23]  John R. Brauer,et al.  Magnetic Actuators and Sensors: Brauer/Magnetic , 2013 .

[24]  B G Fallone,et al.  Magnetic shielding investigation for a 6 MV in-line linac within the parallel configuration of a linac-MR system. , 2012, Medical physics.

[25]  B. G. Fallone,et al.  Design and Optimization of Superconducting MRI Magnet Systems With Magnetic Materials , 2012, IEEE Transactions on Applied Superconductivity.

[26]  B G Fallone,et al.  Three-Dimensional Nonaxisymmetric Pole Piece Shape Optimization for Biplanar Permanent-Magnet MRI Systems , 2011, IEEE Transactions on Magnetics.

[27]  Sasa Mutic,et al.  SU‐E‐T‐352: Commissioning and Quality Assurance of the First Commercial Hybrid MRI‐IMRT System , 2012 .

[28]  Jeffrey C. Lagarias,et al.  Convergence Properties of the Nelder-Mead Simplex Method in Low Dimensions , 1998, SIAM J. Optim..

[29]  Bin Meng,et al.  Short communication A SQP optimization method for shimming a permanent MRI magnet , 2009 .

[30]  B G Fallone,et al.  Effect of longitudinal magnetic fields on a simulated in-line 6 MV linac. , 2010, Medical physics.

[31]  S. Tumański Handbook of Magnetic Measurements , 2011 .