Julian Emmerich1, Sina Straub1, and Frederik Bernd Laun1,2
1Medical Physics in Radiology, German Cancer Research Center (DKFZ), Heidelberg, Germany, 2Institute of Radiology, University Hospital Erlangen, Erlangen, Germany
Synopsis
Due to imperfect laser
positioning, actual isocenter
slicepositions can deviate from manufacturer indication. Using MRI as tool for dose planning in MR guided
radiation therapy, the geometric correct position of MR-slices is an essential
quality parameter that can affect dose calculation and definition of the
planning target volume (PTV). To evaluate the magnitude of the deviation of
the actual slice position from the true isocenter of the scanner, a phantom
study was performed. Scanner-dependent deviations in isocenter slice position
occurred in the range of 1 mm - 5 mm.
Purpose
Using
MRI as tool for dose planning in MR-guided radiation therapy, the correct geometric
position of MR-slices is an essential quality parameter, especially when using
integrated MR/radiation therapy devices1. It can affect dose
calculation and definition of the planning target volume (PTV)2.
To evaluate the magnitude of the deviation of the actual slice position from the
manufacturer indication, a phantom study was performed. The phantom was
designed such that it can be measured “online”, i.e. in parallel with the
patient data acquisition.Methods
A
phantom consisting of a pair of two crossed isosceles right-angled triangles on
both sides (Fig. 1) was used to measure the difference between the slice
positions defined by the vendor-provided laser positioning system and the slice
position defined by the magnetic field gradients. If the MR-slice is located in
the middle-plane of the phantom, both triangles will appear with the same length in
the MR-image. If the slice is shifted, the triangles on both sides (‘right’ and
‘left’) will appear shortened/extended by the length $$$\Delta l$$$. The deviation $$$\Delta z$$$ of the slice
position of a transversal slice can be measured as $$$\Delta z = \Delta l$$$. This device is similar to the test object used
in the phantom of the American College of Radiology3, but the
phantom was designed such that it can be measured in parallel with the patient.
To this end, the
phantom was integrated in a plastic box that could be integrated in the shuttle
table used in a recent MR-guidance study2. The box was filled with
tab water. Measurements were performed at four different MR-Scanners (SIEMENS Symphony
fit 1.5T, Aera 1.5T, Prisma 3T, Biograph mMR 3T). Over a period of four weeks,
the following sequences were tested at each scanner three times a week: TSE (turbo-spin-echo),
FLASH (Fast-Low-Angle-Shot), TRUFI (true
fast imaging with steady-state free precession)
and VIBE (volumetric interpolated breath-hold examination). Automated
data analysis was performed with Matlab (The MathWorks, Inc., Natick, MA, USA).Results
The
time-curves of the deviation of the slice position are shown in Fig. 2. There
is only a rather small inter-day variation in the data. Only for the SIEMENS Prisma,
there is a larger drop in slice position after the third measurement (green
lines in Fig. 2, A-D), which occurred after a recalibration of the system by a
service technician. The scanner isocenter was recalibrated using a spherical
phantom and a build-in software tool on the MR-scanner. The differences in
slice position between the used sequences are smaller than 1 mm and change
only within the standard deviation (except for the Prisma). Mean values of the slice
position are given in Table 1. In Fig. 3, the deviation in slice position is plotted
pairwise for all sequences and all four scanners in scatter plots. There is a
significant correlation between the measurement results for the different
sequences (all correlation coefficients are larger than 0.98 with p <
0.001). The red lines in Fig. 3 indicate a linear fit with slope p1 and
intercept p2 (cf. Tab. 2). In the inter-scanner comparison, there are large
differences between the different scanners of about 6 mm - 8 mm.Discussion
The
dependence of the deviation of the scanner system is much stronger than the
dependence on the sequence indicating that the main underlying reason for the deviation
can be attributed to a scanner specific uncertainties. Due to the weakly
mounted laser positioning systems of the scanners, the laserbeams can be
misplaced by several millimeters by touching the casing of the scanner. This can
lead to a mispositioning of the patients if the casing is displaced accidently.
Slice positioning
errors could be minimized by using a stationary laser positioning system as
used in conventional radiation therapy or by more reliable calibration
procedures4. Conclusions
Deviations
of more than 6 mm occurred in the inter-scanner comparison of four
scanners. Especially when using MR images for radiation treatment planning,
this might not be negligible. With the used setup, consistent absolute image
position cannot be ensured between different imaging sessions. When critical
spatial parameters need to be derived from MR images, e.g. for MR-guided
radiation therapy, better positioning systems and more precise calibration
methods would be valuable.Acknowledgements
No acknowledgement found.References
1. Lagendijk, et al. (2008). MRI/linac
integration. Radiotherapy and Oncology, 86(1), 25-29.
2. Bostel, T. et al. Radiation Oncology (London, England)
9 (2014): 12. PMC. Web. 6 Nov.
2016.
3. Clarke, G. D. (2004). University
of Texas Southwestern Medical Center at Dallas.
4. Brahme, A., Nyman, P., and Skatt, B. (2008). Medical Physics, 35(5),
1670-1681.