Pulkit Malik1, Tracy Wynn1, Peter Fischer1, and Gillian Haemer1
1InkSpace Imaging, Pleasanton, CA, United States
Synopsis
Keywords: RF Arrays & Systems, Data Analysis, Receive Array SNR
We present a MATLAB
based visualization toolbox for locating coil elements and evaluating SNR for
flexible coil arrays. The greater variation in coil positioning creates
challenges for SNR comparisons. By locating coils with coil sensitivity
isocontours, the SNR of individual channels can be evaluated while the coil
array is flexed. This is used to examine the repeatability of placement, and
changes to coil coupling in the different placements. The coil locations can be
validated using the SNR visualization displayed as slices, lines, and probe
points. Expectations of the SNR field shape are used to further optimize coil
locations.
Introduction
Signal to noise
characterization of receive arrays is an important foundation for coil
development and analysis. Flexible receive arrays have received increased
interest for their subject-specific adaptability, patient-friendliness, and
clinical usability1-8. However, repeatable, quantitative SNR
characterization can be challenging.
Changes in individual element positions relative to the subject create a data
registration issue, often mitigated with the use of custom fixturing or
registration algorithms. Because flexible coils are intended to conform to
patient anatomy, positioning the coil around the subject often results in
variations in coil loading and coupling, information which is lost by using
one-size fits all fixtures. In this work we present an SNR toolbox which uses
coil sensitivity mapping to inform the user on coil positioning and loading,
and which generates individual element SNR measurements. This toolbox allows
for SNR comparison on an individual element basis, while generating a visual
representation of element positions relative to the subject.Method
SNR for was first
measured on a 3T scanner by acquiring a 3D spoiled gradient echo
(TR/TE/FA/BW/Res = 140ms/3ms/30°/62.5Hz/[1.25,1.25,2] mm), and an equivalent
noise scan without RF excitation. The data was analyzed in Matlab (2019A) using
the Kellman method9 to output a 3D matrix
in SNR units. The coil images and SNR matrix were used as the input to the
toolbox for SNR visualization and coil position analysis.
Coil locations were
calculated using sensitivity isocontours to estimate a vector normal to the
coil. Centroids of the 3D isocontours were used to perform a linear regression.
The resulting unit vector was used to determine the tilt of the coil, and the
coil was located based on a user-chosen distance from the first isocontour.
After the automated
calculation, the toolbox allows manual adjustment of coil rotation and offset
distance. Individual element SNR is proportional to field strength and falls
off relative to the distance from the coil, so it may be analyzed according to
the following equation, where R is the coil radius and y is the distance to the
coil:
$$\vec{B} = \frac{\mu_0 I R^2}{2(y^2 + R^2)^{3/2}}\hat{\mathit{j}}$$
By evaluating SNR along the normal vector
relative to the equation above, the position and angle of the vector may be
optimized to best suit the data, including a global correction for B1 twist.
After coil positions,
normal vectors, and isocontour plots have been calculated, the visualization is
generated. The combined SNR image is visualized in 3-dimensions using 2D
sagittal, coronal, and axial slices. Slice positions can be adjusted to
visualize the entire volume. SNR line profiles along plane
intersections are plotted to visualize the overall shape
and level of SNR through the phantom. Finally, for each coil a probe into the
volume along the normal vectors is shown and used to calculate a point SNR
measurement at a given depth to provide quantitative measurements for each
channel. Isocontour plots can be displayed within the visualization and may be
used to optimize coil locations and compensate for B1 twist (LISA artifact).Discussion
SNR comparisons of flexible coils are often
performed on flat phantoms to minimize variations in coupling between elements
and in coil loading, and to allow for easy analysis of SNR in a 2D slice at a
set distance from the array. However, variations in coupling and loading based
on positioning is an intrinsic part of a flexible coil’s SNR that should be
captured in analysis, and evaluating coils in a wrapped geometry for various
applications is often important. The purpose of this SNR toolbox is to
effectively compare SNR of flexible coils in representative positions for
varying use cases. By locating and visualizing individual elements’ SNR, we
hope to move closer to a quantitative and fair comparison tool between flexible
coils and non-flexible industry standard arrays, taking loading and coil
positioning into account.
Further refinement of
this toolbox is in progress to make it a more powerful tool. First, the
visualization tool currently uses a sum-of-squares based SNR calculation.
Adding a more complex SNR processing tool to utilize coil sensitivity maps may
improve analysis of coil coupling. Second, manual adjustment of the normal
vector for individual elements relative to the expected profile will be upgraded
to include a gradient descent aided optimization to improve usability. Third,
automated calculations of B1 twist, based on known properties will be included
to improve coil visualization. Finally, phase maps of the
coil array generated via the body coil could provide detailed information about
coil orientation.Conclusion
This toolbox is still in
the early stages of development, yet it has already been useful in identifying
global variations in coil positioning.
Day-to-day variations in coil positioning have been confirmed by the automated
coil position visualization of the SNR. As the toolbox is used and updated, we
expect to minimize variation in SNR measurements between setups for our
flexible arrays. Acknowledgements
This work was supported in part by NIH grant R44 EB028728-03.References
[1] Nordmeyer-Massner, et al; MRM 2009. 61(2):429-38.
[2] Corea, et al; Nat Commun 2016. 7: 10839.
[3] Rossman, et al; ISMRM 2017: p763.
[4] Frass-Kriegl, et al; PLoS One 2018. 13(11): e0206963
[5] McGee, et al; Phys Med Biol 2018. 63(8): 08NT02.
[6] Zhang, et al; Nature Biomed Eng 2018. 2(8): 570-7.
[7] Zhang, et al; MRM 2019. 81(5): 3406-15.
[8] Collick, et al; Phys Med Biol 2020. 65(19): 19NT01.
[9] Darnell, et al; JMRI 2021. 55(4): 1026-42.
[9] Kellman, et al; MRM, 2005. 54(6): 1439-47.