HAMZA RAKI1,2, SIMON A. LAMBERT1, KEVIN TSE VE KOON1, HENRI SOUCHAY2, FRASER ROBB3, ISABELLE SANIOUR1, and OLIVIER BEUF1
1Univ. Lyon, INSA-Lyon, Université Claude Bernard Lyon 1, UJM-Saint Etienne, CNRS, Inserm, CREATIS UMR 5220, U1206, F-69000, LYON, France, 2General Electric Healthcare, Buc, France, 3General Electric Healthcare, Aurora, OH, United States
Synopsis
Single-loop endoluminal
RF-coils are a possible solution for the SNR limitations of external coils.
However, they suffer from signal variations due to the coil sensitivity
dependence with the coil orientations with respect to the B0 field.
We simulated (electromagnetic simulations with Feko) an RF-coil along the Ox
axis (0°) taken to be that of the B0 field and for specific coil
orientations (30, 45, 60 and 90°) around and in oblique position with respect
to the Ox axis (B0). We then evaluated the signal distribution
(H-field 2D map) variation with the coil orientations to can propose an
adequate architecture.
Introduction
Magnetic Resonance Imaging
(MRI), based on an array of external receiver coils, is usually used for
medical diagnosis of abdominal and gut diseases to provide an improved Signal-to-Noise
Ratio (SNR). However, the latter is not sufficient to depict thin bowel and
colon wall1. For this purpose, previous works
have demonstrated the value of internal (endoluminal) coils close to the region
of interest2–4. However, single-loop endoluminal
RF-coils suffer from the signal variations due to the coil sensitivity
dependence with various possible coil orientations with respect to the magnetic
field B05. In fact, a single loop RF-coil has a
maximal sensitivity when its axis is aligned with the main magnetic field B0
(The RF B1 is orthogonal to the B0). This is considered
as the reference orientation. In all other orientations of the coil, the signal
distribution changes; thus the sensitivity and subsequent image quality
decrease. This is a major challenge in clinical colon diagnosis. One solution
is the development of endoluminal RF-coil based on the combination of different
loops to be able to cover different orientations. The purpose of this work was
to simulate, the effect of different orientations of the RF-coil with respect
to the B0-field on the signal distribution.
Methods
We simulated using a
commercial electromagnetic software based on the moment method (Feko) a
rectangular-loop (5.1x47 mm2)
endoluminal receiver coil. The Ox axis was taken to be that of the B0
field and aligned along the length of the coil (fig. 1a). Other orientations
were simulated by rotating the coil either about the Ox axis (45 and 90°) (fig.
1b), the Oy axis (fig. 1c) or the Oz axis (fig. 1d). Then the magnetic field
(H-field) 2D-maps (slice perpendicular to the plane of the coil) were extracted
considering only the components perpendicular to the direction of the B0
(i.e. Ox) that can probe the transverse magnetization.
Results
Simulations showed that
rotating the coil around the Ox axis
do not change significantly signal distribution (fig. 2b) compared to the
reference orientation (0°) (fig. 2a). This was different when the coil is rotating around
the Oy or Oz axis where large
variations of the signal distribution were observed. For a 90° angle around the
Oy or Oz axis, signal distribution
is a four-leaf clover shape with cancelation along diagonals (fig. 2c,d).
Discussion/Conclusion
These preliminary results
show the dependence of the signal distribution of the coil as a function of the
orientation of the coil with the B0 field. Large variations occur
when the coil is perpendicular to the main magnetic field B0
(four-leaf clover shape). These variations degrade the coil sensitivity. Reconfigurable-loops
geometries could provide a solution to minimize the loss of signal and maximize
the homogeneity. Further work will work with architecture which is able to
operate in several orientations and we will investigate reconfigurable coil
made of different elements by using Micro Electro-Mechanical System (MEMS)
switches, developed by GE Healthcare, to activate some loops and deactivate
others to operate in any orientations with optimal sensitivity.
Acknowledgements
Authors would like to
thank the LABEX PRIMES of University of Lyon, which has supported this work
within the program "Investissements d'Avenir" (ANR-11-IDEX-0007)
operated by the French National Research Agency (ANR).References
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