Bu S Park1, Sunder S Rajan2, and Brenton McCright1
11Division of Cellular and Gene Therapies, FDA/CBER/ Office of Tissues and Advanced Therapies, Silver Spring, MD, United States, 2Biomedical Physics, FDA/CDRH/Office of Science and Engineering Laboratories, Silver Spring, MD, United States
Synopsis
We present numerical
simulations and experimental
validation data testing the feasibility to
improve 19F image sensitivity of perfluorocarbon labeled cells using
the secondary resonator tuned at 287 MHz to make an enhancing induced RF
magnetic field (B1) at
7.0T 19F/1H MRI. The
numerical simulation results of |B1+| and
corresponding experimental 19F images without and with the secondary
resonator tuned at 287 MHz show the improvement of |B1+|
and 19F image uniformity. To model a potential clinical application,
we used inductive coupling MR to image 19F perfluorocarbon labeled
cells encapsulated in polyethylene glycol (PEG) after their transplantation
into mice.
Introduction
Commercially available transmit and receive
surface coils often have simple planar designs that have a rapid fall-off in
sensitivity with depth. Such limited radio frequency (RF) magnetic field (B1) uniformity is
problematic when attempting to image even relatively small volumes of an animal
anatomy. In our study, we demonstrate how the addition of a separate secondary
resonator located beneath a commercial coil can provide uniform images of 19F
nuclei with high sensitivity. Numerical simulations and experimental validation
results show that the “secondary resonator” can be used to improve or worsen
the image uniformity and sensitivity of 19F MRI.
Methods
All experimental measurements were performed using
an Agilent 7.0T horizontal bore animal MRI (Agilent Inc., Santa Clara, CA) with
an open bore of 310 mm, a diameter of 115 mm inside the gradient coil
(Resonance Research Inc., Billerica, MA). The commercial surface coil used for
all experiments was a dual-tuned 19F/1H surface coil
(RAPID MR International Inc., Columbus, OH). The secondary resonator (inner
diameter (ID) = 18 mm, outer diameter (OD) = 22 mm) was tuned either to 287 MHz
or 277 MHz with capacitors equal to 4.7, 5.5, and 11 pF (ATC Inc., Huntington
Station, NY) combined with a variable capacitor to produce either an enhancing
or an opposing RF magnetic field in the secondary resonator (B1L). A polyethylene glycol (PEG)
disk with a diameter of 6 mm containing 12´106
19F labeled neural stem cells (NSCs) encapsulated in PEG following
methods adapted from established protocols (1) was inserted subcutaneously in
the back of a NSG mouse. The transplanted NSCs expressing luciferase were
detected by bioluminescence after intraperitoneal injection of luciferin using
the IVIS® SpectrumCT (PerkinElmer Inc., Waltham, MA). Numerical simulations were performed
using the xFDTD software (Remcom Inc.,
State College, PA) and post-processing analysis was performed in Matlab (MathWorks
Inc., Natick, MA). All
the simulation results were normalized to obtain a magnitude of the transmit RF
rotating magnetic field (|B1+|) equal
to 2 mT at
the center of the phantom.Results
The |B1+|
uniformity was improved when the resonator was tuned at 278 MHz (fL)
with CL of 16.8 pF (Fig. 1, second column), whereas it becomes worse
when fL was 277 MHz with CL of 18.0 pF (Fig. 1, third
column). It shows that the enhancing induced B1+ would be produced when the secondary
resonator was tuned at higher frequency compared to the resonance frequency of
the 19F surface coil, fo of 282 MHz (Fig. 1, second column, WithE). Conversely, the
opposing induced B1+
was produced when fL was lower than fo (Fig. 1, third column, WithO). Because the NSCs expressed
the luciferase gene, the location and viability of the implanted cells could be
monitored by luminescence over a period of 6 weeks (Fig. 2 (b)). MRI detection
of the cells in vivo was done without (Fig. 2c, first row) and with (Fig. 2c, second
row) the secondary resonator tuned at 287 MHz to make enhancing magnetic
fields. The use of the resonator improved our ability to visualize transplanted
cell location and survival non-invasively over a period of 6 weeks.Discussion
When
comparing to the results available in literature related to our study of inductive
coupling (2-3), our study presents the following novelties: 1)
numerical simulation results of |B1+|
and ÐBY (Fig. 1 (b) and (c)) without and with the secondary
resonator designed for 19F imaging at 7.0T generated enhancing
(second column) or opposing (third column) induced B1L depending on the
tuning status of the resonator; 2) the method used in our study was based
on in vitro and in vivo experimental results from a model clinical application,
19F labeled stem cells encapsulated in PEG (Fig. 2); 3) The in vivo
MR imaging of encapsulated NSCs is a novel and potentially clinically relevant
application of 19F MRI (Fig. 2). The use of a secondary resonator
could be generally applicable in other similar situations where the available
RF surface coil does not provide the desired image quality.
Disclaimer: “The mention of commercial products, their
sources or their use in connection with material reported herein is not to be
construed as either an actual or implied endorsement of such products by the
Department of Health and Human Services.”
Acknowledgements
No acknowledgement found.References
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J. J Vis Exp. 32, 1-5, 2009 2. Merkle H et al, MRM 66:901–910, 2011 3. Schnall et al., JMR 68:16 l-167, 1986