Synopsis
We
have developed a single-shot 3D sequence for hyperpolarized 13C MRI,
with a spatial-spectral (SpSp) pulse for excitation and a stack-of-spirals
acquired in interleaved fashion during two spin echoes. The sequence achieved a
resolution of 1.25x1.25x2.5 mm3 in vivo on a 7T animal system, where
hyperpolarized [1-13C]pyruvate and [1-13C]lactate were
imaged alternately at a frame rate of 2 s per metabolite. Variations are
allowed in the design of the acquisition train to balance the in-plane and
through-plane resolutions. This sequence allows higher temporal resolution and
less RF depletion of the polarization than pulse sequences described previously.Purpose
Development of a hyperpolarized
13C
MRI pulse sequence for acquiring high-resolution 3D images after a single excitation.
Introduction
Imaging
tumour responses to treatment through changes in metabolism can be advantageous
as the morphological changes observed using traditional imaging methods can be
slow to show evidence of a treatment response. Imaging of
13C-labelled
cell substrates has become a promising technique for tumor treatment monitoring
with the development of DNP in the past few years
[1]. However, the
hyperpolarization is transient, limiting the imaging time and number of
excitation pulses in the experiment. We describe here a single-shot 3D imaging
sequence to image hyperpolarized
13C-labeled substrates at high
resolution, both spatially and temporally.
Method
The
sequence is shown in Figure 1. Following each SpSp excitation pulse, the pulse
sequence acquires a stack-of-spirals such that each kx-ky plane, in 3D k-space,
is acquired with a spiral-out trajectory and the blipping gradient train
encodes the spatial information in the z-direction. The spirals are interleaved
to reduce the impact of system imperfections. The two pairs of Hyperbolic-Secant
adiabatic inversion pulses form two spin echoes, which are acquired by the two
central spirals, enhancing the overall SNR while reducing polarization
depletion due to imperfect refocusing pulses. The design of the spiral trains can
be varied depending on the requirements of the application: as displayed in Figure
1, acquiring larger matrices at the center of k-space and smaller ones at the periphery
yields a 3D k-space with a near-spherical stack-of-spirals. Alternatively an
identical matrix size for all kx-ky planes can be used, resulting in a
cylindrical stack-of-spirals. Different designs result in different 3D point
spread functions; choosing between them can be used to balance the in-plane
resolution against the through-plane resolution.
Experiments
Experiments were performed on a 7T scanner with
3 female C57BL/6J mice bearing EL4 lymphoma tumours. Imaging commenced just
before intravenous injection of hyperpolarized [1-
13C]pyruvate, with
a FOV of 4x4x2 cm
3 and a nominal resolution of 1.25x1.25x2.5 mm
3.
The 1/3/5/7 (or, identically, 8/6/4/2) spirals
[2], as shown in Figure 1,
encoded matrix sizes of 4x4, 16x16, 32x32, 8x8, respectively. The spiral
lengths, in the same order, were 0.656, 3.240, 8.580, and 1.344 ms. The SpSp
pulse had a bandwidth of 350 Hz, a stop band of 1295 Hz, and a total duration
of 10.056 ms. The flip angle was 15⁰ on pyruvate and 90⁰ on lactate, following a saturation-recovery scheme
[3]. The TE1 and TE2,
as indexed in Figure 1, were 50.6 ms and 110.504 ms respectively. The SpSp
pulse was targeted alternately at the pyruvate and lactate resonances, giving a
temporal resolution of 2 s per metabolite (TR = 1 s), while the total
acquisition window was 60 s. Phase correction
[4] was performed before the
reconstruction process to remove the gross phase inconsistencies between each
acquired spiral.
Results
The
time courses of the signals from pyruvate and lactate are shown for all 3 mice
in Figure 2, and were calculated by summing the signal from all the pixels in
the 4
th slice. Lactate signal intensity was tightly correlated with the
pyruvate signal strength, because the accumulation of lactate signal between
excitations was prevented by the use of a 90⁰ flip angle pulse on the lactate resonance. The
pyruvate and lactate images from the 4
th slice, overlaid on the
proton Fast Spin Echo (FSE) image at the same position, are shown in Figure 3
for one mouse, between 0 s and 29 s. For the same mouse, the pyruvate and
lactate signals are displayed in Figure 4 for all 8 slices at 6 s and 7 s
respectively, overlaid on the proton FSE images. Tumour heterogeneity can be
observed from the inhomogeneous distribution of the pyruvate and lactate
signals.
Discussion and conclusion
The proposed pulse sequence is, to the authors’
best knowledge, the first single-shot 3D sequence for hyperpolarized
13C
MRI. The single-shot scheme can dramatically reduce the required number of
excitations compared to earlier 3D techniques. Compared to 2D imaging methods,
the sequence is beneficial in terms of both the reduced number of excitations
and higher SNR. It has been shown to be capable of imaging exchange of
13C
label between injected [1-
13C]pyruvate and endogenous lactate in
vivo at high spatial and temporal resolutions. Variations in the design of the
spiral train allow different trade-offs between the in-plane and through-plane
resolutions. The total duration of the sequence is much smaller than the TR
used, leaving room for higher temporal resolution if required.
Acknowledgements
No acknowledgement found.References
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Brindle KM. Imaging metabolism with hyperpolarized 13C labeled cell
substrates. J Am Chem Soc 2015;
137:6418-6427
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412-415
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Ardenkjaer-Larsen JH, Glaser SJ, Haase A, Schwaiger M, Wiesinger F.
Saturation-recovery metabolic-exchange rate imaging with hyperpolarized [1-13C]pyruvate
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