Yaohui Wang1, Qiuliang Wang1, Jigang Zhao1, Yang Liu1, Yijie Zheng1, Zhifeng Chen2, and Feng Liu3
1Institute of Electrical Engineering, Chinese Academy of Sciences, Beijing, China, 2USC Stevens Neuroimaging and Informatics Institute, Keck School of Medicine, University of Southern California, Los Angeles, CA, United States, 3School of Information Technology and Electrical Engineering, The University of Queensland, Brisbane, Australia
Synopsis
A small-size, light-weight, cryogen-free 7T animal MRI system is being
developed in IEE CAS. The magnet system has been completed and acceptable
magnetic field strength and homogeneity indices have been achieved. The
gradient assembly with passive shimming is going into the final assembly stage
and the RF coil is ready for tunning. The integration of the whole system will
be very soon and a mouse experiment will be conducted then. It is expected the
ultimate product will largely boost the scientific research activities that are
unapproachable to advanced MRI scanners.
Introduction
High-field
MRI has significant advantages in terms of signal to noise ratio (SNR) and
resolution, which can not only image the microscopic structure of biological
tissue, but also explore the cognitive function, and even conduct metabolic
detection of the living body [1]. However, existing
high-field MRI systems usually have a bulk volume with a vast amount of liquid
helium stored, having a high fabrication and maintenance cost beyond the budget
of many MRI users. In this work, a small-size, light-weight, 7T cryogen-free
animal MRI scanner is under development in the Institute of Electrical
Engineering, Chinese Academy of Sciences (IEE CAS). Until now, the
fabrication of the superconducting magnet of this Benchtop 7T system has been
completed, the gradient coil is in the final assembly stage, and the RF coil is
ready for tuning. We report here on progress details of the hardware system development.Method
In designing the actively-shielded superconducting magnet of the Benchtop
7T MRI system, we adopted a radial current density classification scheme by
using different wire gauges on the primary long solenoid coils [2]. Based on the magnetic field of the primary
coils, several adjusting coils were necessary to elevate the central field
strength further and offset the unwanted inhomogeneous magnetic field
components simultaneously, and shielding coils were used to constrain the
5-Gauss line range. The magnet was wound with NbTi superconducting wires on
aluminium alloy bobbins to guarantee a large heat transfer coefficient. Oxygen-free
copper was used as the conduction tape connected to a pulse tube cryocooler [3]. The magnet coils were hoisted in a helium-free
cryogenic vessel and operated in a dry mode. Inside the warm bore of the
magnet, a thin gradient assembly will be installed. The three-axis gradient
coils were all unshielded to reduce the total thickness, where a hollow z
gradient coil also plays a role of cooling pipe, and the shim trays were placed
in the inner wall of the coil bobbin. A relatively large available space will
be reserved to install the RF coil and then use for the imaging detection.Results
The coils structure of the main magnet is illustrated in Fig. 1, which
includes five primary coils 1-5, four adjusting coils 6-9, three shielding
coils 10-12, and three electromagnetic interference screening (EIS) coils 13-15
[4]. The fabricated magnet coils, heat conduction
structure, cold shield and vacuum container are shown in Fig. 2. The magnet was
dedicatedly protected with thermal insulation, and one pulse tube cryocooler
was directed and connected to the magnet endplate.
The final magnet system was tested, as shown in Fig. 3, and specified magnet
strength and homogeneity were achieved. The magnet has a dimension with a length
of 635mm, width 490mm, and height 883mm, the horizontal warm bore diameter is
54mm with 30mm DSV, and the total mass of the magnet is 255kg. The temperature
of the magnet coils was cooled to less than 4K in a steady state.
The gradient assembly design is illustrated in Fig. 4, where the
integral scheme is presented in Fig. 4(a), the layout of the assembly structure
is diagrammed in Fig. 4(b), the designed coil patterns are plotted in Fig.
4(c-e). The engineering components of the assembly are shown in Fig. 4(f-i). A
passive shim tray with 14 strips in the circumferential direction and 34 in the
axial direction was embeded in the substrate. The transverse gradient coils will
be cut out on the copper plates, and the axial gradient coil was wound with a hollow
copper pipe. The outer diameter of the gradient assembly is 53mm, leaving a 1-mm
assembling gap to the magnet warm bore, and the inner diameter is 40.68mm.
The
RF coil adopts a birdcage structure with eight legs, and there are six
capacitors at one end ring and eight capacitors at the other. The capacitors
have an identical capacitance of 23 pF and contribute a resonance frequency
299MHz.
The main parameters
of the Benchtop 7T cryogen-free animal MRI system are listed in Table I.Discussions
Since
the gradient coils were not actively shielded to enlarge the available
detection bore size, we will be very careful of using a fast scanning sequence.
The relatively slow sequences are workable based on our previous experience due
to weak eddy current, and the follow-up study on the image correction method
under fast imaging is essential to support more sequence requirements.
Alternatively, we will also consider the actively shielded gradient coil
design.Conclusion
A Benchtop 7T cryogen-free animal MRI system is under development at IEE
CAS, whose clear detection bore diameter is around 32mm, which is feasible for
the imaging of small-size organisms, such as mice. Significant merits of the
system include cryogen-free operation, small magnet size, light weight, etc.,
which result in very high performance to cost ratio. The ultimate product is
expected to boost a wide range of scientific research programs that require
ultra-high-field MRI technology.Acknowledgements
This work is
funded by CAS Pioneer Hundred Talents Program (Grant No. Y8402A1C31) and National
Key Research and Development Program of China (Grant No. 2020YFF01014702).References
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