Passive magnetic shielding for in-beam MR imaging during proton pencil beam irradiation


Passive magnetic shielding for in-beam MR imaging during proton pencil beam irradiation

Semioshkina, E.; Oborn, B.; Hoffmann, A. L.

Introduction
Dynamic magnetic fringe fields produced by the scanning magnets (SMs) of a proton pencil beam scanning (PBS) research beamline have shown to cause severe image artefacts during in-beam MR imaging [1]. In this study we investigate the effect of different design parameters of a passive magnetic shield positioned around the SMs on the reduction in magnitude of the magnetic fringe fields the SMs produce.

Methods
A finite element model of the PBS beamline was used to calculate the magnetic fringe fields produced by the SMs. Parameters investigated for a carbon steel magnetic shield included: geometry, material thickness, number of material layers, size of the air gap between layers. The shielding factor (SF) at the projected position of the MR isocenter was calculated. Previous measurements at our facility showed that a SF of at least 20 is required for artefact-free MR imaging during PBS dose delivery.

Results
A cost-efficient way to achieve the required SF was to use a multilayer cylindrical shield. A SF of 21 was achieved for two concentric layers of 10 mm thickness with a 10 mm air gap. The SF can be further increased to 25 by an additional layer. Setting the air gap equal to the layer thickness gave the highest shielding performance.

Conclusion
Computer simulations showed that a passive magnetic shield around the SM can provide the required SF using a multilayer cylindrical geometry with an interlayer air gap equal to the layer thickness.

References
[1] S. Gantz et al. 2020 Phys. Med. Biol.

  • Contribution to proceedings
    The 59th Annual Conference of the Particle Therapy Co-Operative Group (PTCOG 59), 04.-07.06.2021, Online Meeting, Online Meeting

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