Junnan Wang1, Rongsheng Lu1, Layale Bazzi2, Xiaowen Jiang1, Yi Chen1, Zhengxiu Wu1, Qing Yang1, Zhonghua Ni1, Hong Yi1, and Dan Xiao2
1School of Mechanical Engineering, Southeast University, Nanjing, China, 2Department of Physics, University of Windsor, Windsor, ON, Canada
Synopsis
The permanent magnet based low-field and low-cost
MR systems increase the accessibility and potential of point-of-care diagnosis,
where relaxometry measurement is usually preformed due to the low requirement
of B0 field homogeneity. However, inhomogeneous B1 field results
in errors in the T2 relaxation times, especially in in-vivo
localized human tissue measurements. A novel RF coil termed T coil has been developed
to provide a better B1 field homogeneity and more accurate in-vivo relaxation
measurements than the conventional coils. This may enable the noninvasive
diagnosis of diseases through the human finger measurements with portable and
affordable MR systems.
INTRODUCTION
Metabolic
syndrome has affected human health seriously, with an increasing incidence rate1.
Early detection and intervention are important to reduce the prevalence of
metabolic diseases2-4. Low B0 field MR detection has
become a popular research topic due to the low cost and portability. The
permanent magnet based low field studies mainly focus on analyzing the T1
and/or T2 relaxation times, termed relaxometry5-6, to
quantify the multiple microscopic components. In contrast to chemical shift
spectroscopy, an accurate transverse relaxation experiment requires high
quality 180°
refocusing RF pulses for the entire effective volume. In the finite region,
where B1 field transitions from the maximum value to zero, tissues
experience nonideal refocusing pulses leading to errors in the measured T2
values, especially for the components with T1 much greater than T27.
In this paper, the RF coil was optimized to provide a B1 field with
improved homogeneity to increase the accuracy of multicomponent relaxation
measurements.METHODS
T coil with improved B1 homogeneity
Alternating current accumulates
at the edge of the copper foil parallel to the direction of current flow, improving
the uniformity of the B1 field. In this work, the loop-gap coil is
modified with additional thin strips, termed T coil (Fig. 1), to further optimize
current distribution and B1 field homogeneity. The finite element
analysis method8-9 was employed to simulate the B1 field distributions.
FID
experiments with small flip angle were simulated (Python, ver. 3.7) and
performed at 10MHz with a thin slice phantom to verify the B1 field
distribution.
The T coil was compared
with a regular solenoid coil and a variable width coil, in all the simulations
and MR experiments.
Phantom and in-vivo relaxation experiments
The complex
human tissue is represented by a silicon rubber phantom, where multiple MR
relaxation components exist due to its cross-linking states and different chain
lengths. The CPMG signals were simulated with the Bloch equation. Relaxation
experiments were performed on a thin slice phantom and a phantom similar to the
size of a human thumb, to investigate the effects of B1 fields. The in-vivo 2D T1-T2
relaxation correlation experiments of human thumb were implemented with the T
coil and conventional coils.RESULTS
The simulated B1 field
distribution of the conventional and T coils are shown in Fig.2. Superior B1 homogeneity
was achieved with the proposed T coil. The B1 field distribution was
validated with the FID simulations and experiments in Fig.
3.
The inhomogeneous B1 fields led to non-ideal RF refocusing
and large errors in the CPMG experiments for short T2 and long T1
components. The thin phantom experiments quantitively evaluated errors at different
positions of the coils (results not shown). The large
phantom had a reduced quantity of the fastest T2 component,
most severe with the regular coil where the shortest
T2 peak area was
32% lower than the true quantity (Fig.4). The T coil
generated a T2 distribution closest to the true spectrum. The
fastest relaxing peak area had a relatively low error of 8%. The in-vivo
results agreed with that of the large silicon phantom (Fig. 5). The quantity of
the shortest T2 component was largely underestimated with the
regular coil and variable width coil.DISCUSSION
The
substances with weak spin-spin interactions, such as liquid molecules,
generally have the same T1 as T2. The CPMG results are
less affected by the RF pulse flip angle and B1 inhomogeneity.
However, large errors may occur with and non-ideal refocusing, where the decay of
transverse magnetization depends on both T1 and T27.
The acquired effective T2 deviates from the true T2 value
$$ 1/T2,eff = 1/T2-<nz2>(1/T2-1/T1) (1) $$
where <nz2> is a constant representing the degree of B1
field inhomogeneity. Amongst the three coils investigated in this work, the
regular coil has the largest <nz2> value, and the T coil has the smallest <nz2> value. When the sample T1 is much
larger than T2, the difference between the acquired effective T2
and the true T2 value is significant with a large <nz2>. The
simulations and phantom experiments verified that the proposed T coil improved
B1 field homogeneity and reduced T2 errors, which should
lead to an increased MR detection accuracy of in-vivo finger measurements.CONCLUSION
A
novel coil structure termed T coil was developed in this work. The T coil
provided better B1 field homogeneity than the conventional coils.
The adverse
effects of B1 field inhomogeneity on relaxation component analysis
were validated by phantom relaxation experiments and in-vivo human finger
experiments on a 10MHz permanent magnet system. The
high B1 field homogeneity of the T coil improved the detection
accuracy and may enable the noninvasive diagnosis of diseases through the finger
measurements on low-field, low-cost and portable MR systems.Acknowledgements
The authors thank the
financial supports from National Key Scientific Instrument and
Equipment Development Project of China under Grant No. 51627808, National Natural Science Foundation of China under Grant No. 52075098 and Grant
No. 51605089. D. X.
thanks NSERC Canada for a Discovery Grant.References
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