Aluminum and copper conductors are compared for constructing radiologically transparent MRI surface coil detectors for use in a hybrid MRI - linear accelerator. Radiation dose to skin can cause serious reactions and skin dose is enhanced when materials are placed in the radiation beam. Therefore increases in skin dose due to surface coils must be minimized by optimized construction. A copper conductor causes a three-fold increase in skin dose compared to a similar thickness aluminum conductor. An aluminium coil (20μm thick) was used to image a phantom, yielding 93% of the SNR achieved with a copper tape coil (32μm thick).
The linac-mr combines the treatment capabilities of a linear accelerator (linac) and the imaging capabilities of MRI, making real-time image-guided adaptive radiotherapy possible (see Figure 1)1 . However, radiation dose to the skin is enhanced by materials (especially high-density metals like copper) placed in the radiation beam’s path2, which can cause serious reactions3. Therefore, to take advantage of the high signal-to-noise ratio (SNR) provided by surface coils and arrays4, an optimized design is required to minimize increases in skin dose, while sacrificing as little SNR as possible. Aluminum has been investigated for low-attenuation of kV photons by coils used in an x-ray/MR system5, but the skin dose effects due to high-energy (MV) radiation have not been investigated for aluminum coils.
In this work we compare the performance of aluminum and copper coils in terms of skin dose and image quality.
A 6MV beam linac and a parallel plate ion chamber were used to measure increases in surface dose due to sheets of aluminum, copper, and insulating Styrofoam (5 mm thick) relative to the open beam. The dose under a patient gown was also measured as a reference for skin dose increase. A 0.2 T magnetic field was generated with a double donut magnet to simulate the electron trapping effect of the MRI system’s field. The skin dose is given as a percentage of the maximum dose (Dmax, which occurs at a depth of dmax – see Figure 2).
To characterize the impact of conductor thickness and material on SNR, coils were constructed from aluminum foils (8. 9, 12.5, 12.7, 15 and 20 μm thickness), copper tape (32μm), flexible PCB (17μm), and copper wire (2.05mm diameter). The coils were all 15 × 15 cm2 square loops of 6 mm-wide strip conductors with 12 cm connections to a matching network.
Each coil was tuned to 20.56 MHz (f0) and matched to 50Ω. Loaded and unloaded quality factor (Q) were determined with a VNA S21 measurement using a small probe. Efficiency was calculated6:
$$\eta = 1- \frac{Q_{L}}{Q_{U}}$$
The efficiency predicts how much of the intrinsic SNR can be achieved with the coil6:
$$SNR=\sqrt{\eta}*iSNR$$
A thickness of aluminum was selected that increases skin dose less than a gown pocket while preserving as much SNR as possible. This aluminum coil and a standard copper coil were tested on a phantom in a 0.5 T linac-mr system7. Single slice (20mm thick) images were acquired with a spin-echo (20ms TE) T1-weighted sequence (416ms TR) to measure SNR.
As expected, thicker metal foil causes a greater skin dose increase because there is more material for radiation to interact with. Furthermore, copper interacts more with the beam than aluminum because of its higher density and atomic number.
Thicker copper conductors have increased SNR efficiency because of lower resistance than thin aluminum. Nevertheless, an approximately 17-μm-thick aluminum coil will achieve 90% of the SNR of the copper tape coil. Keeping in mind that foam insulation required for RF safety increases dose by 4%, to have the same impact as a gown pocket (5.2% skin dose increase) the maximum conductor thicknesses are 21.0 μm of aluminum or 7.2 μm copper (1.2% skin dose increase). A 7.2 μm copper coil will provide far poorer SNR than 21 μm aluminum.
The aluminum coil (20μm thick) achieved 93% of the SNR of the copper coil (32μm thick), slightly lower than the predicted 96%. This may be due to limitations in coil construction, set-up uncertainty, and variations in scan calibrations.
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Figure 3: This figure shows the skin dose increase when different thicknesses of copper and aluminum are placed in the radiation beam, including the effect of a 0.2 T magnetic field parallel to the beam. The different slopes of the linear fits highlight the reduction in skin dose achievable with aluminum instead of copper, i.e., the skin dose increases 2.9 times more with copper than with the same thickness of aluminum.