Luis A Loza1, Stephen J Kadlecek1, Mehrdad Pourfathi1, Kai Ruppert1, Tahmina S Achekzai1, Ian F Duncan1, and Rahim R Rizi1
1Radiology, University of Pennsylvania, Philadelphia, PA, United States
Synopsis
129Xe’s
high solubility in tissue and blood, coupled with its dramatic change in
chemical shift based on local chemical environment, enables quantitative
measurements of blood oxygenation. In this work, we demonstrate a technique for
distinguishing oxygenated vs. deoxygenated blood in the mouse circulatory
system in vivo. Time-resolved
dissolved-phase images and spectra were used to identify spectral signatures
for 129Xe dissolved in oxygenated and deoxygenated blood, which were then
applied to a mouse model of lung cancer to temporally assess regional changes
in pulmonary blood oxygenation. The results presented here demonstrate
Introduction
While
hyperpolarized 129Xe (HXe) MRI has primarily been used to study lung
function due to its high solubility in blood and tissue, other potentially
valuable applications include renal perfusion imaging1 and
quantitative measurements of blood oxygenation2. In this study, we
used a modified chemical shift
imaging (CSI) sequence to acquire time-resolved images3 in order to
distinguish between HXe dissolved in oxygenated vs. deoxygenated blood in vivo. This ability to measure
real-time regional blood oxygenation could be valuable for studies of cancer,
ischemia/hypoperfusion and other disease models.Methods & Materials
Genetically
modified C57BL/6 mice (n = 4) were induced with lung cancer as previously
described4 and anesthetized using 1-2% isoflurane; they were then
imaged in a 9.4T vertical-bore micro-imaging MRI system (Bruker Inc.) while
free-breathing a normoxic gas mixture consisting of O2, isoflurane,
and HXe gas administered using a homemade gas delivery system. Image sets were
acquired using a respiratory-gated CSI sequence combined with a user-defined
phase-encode/flip-angle table; HXe distribution at different points in the
circulatory system was visualized by varying the flip-angle (FA) and keeping
the repetition time (TR) constant (FA = 6°, 12°, 25°, 50°, 90°; TR = 80 ms).
Images were reconstructed using the respective flip-angle/phase-encode tables,
and were corrrelated to an effective HXe RF-induced T1 decay value,
T1,RF3, enabling temporal comparison between each image.
As T1,RF increased, so did the complexity of the spectra and
appearance of HXe signal. Given both the temporal and spatial information from
CSI-acquired images, HXe resonances in the blood were assigned a certain
chemical shift based on its appearance in the images and associated spectral
contribution.Results
Figure
1A shows a representative image set of HXe dissolved in the narrow component of
the blood resonance for a wide range of T1,RF values (0.08 s to 14.6
s, in this case). The chemical shift of HXe dissolved in oxygenated blood (HXe
in the aorta/left ventricle) was measured to be +194.5 ppm with respect to the
gas peak, while HXe in deoxygenated blood (HXe in the vena cava/right
ventricle) presented a chemical shift slightly to the left at 195.5 ppm. Figure
1B shows HXe spectra for the same T1,RF range as in Figure 1A (short
to long T1,RFs from bottom to top) for the two regions of interest
(ROI) in the inset, corresponding to a lung tumor (blue) and the left ventricle
(red). The spectra for the ROI in the left ventricle presents a resonance at
194.8 ppm that increases in amplitude with T1,RF; the spectra for
the ROI in the lung tumor also shows a resonance at 194.8 ppm, while a more
prominent resonance at 196.2 ppm increases in amplitude with increasing T1,RF.Discussion
The
technique demonstrated here relies largely on the acquisition of images at
different T1,RF3 values, which not only enables
visualization of HXe distributed at different spatial points within the
circulatory system but, when combined, can also be used to isolate the many
distinct dissolved HXe spectral signatures in differing anatomical compartments
of the mouse body5. Figure 1A shows this spectral isolation
implemented for HXe dissolved only in the blood, while Figure 1B shows
temporally-resolved dissolved-phase HXe spectra for two different ROIs (see
Results). The spectra in the red ROI behave as expected: the resonance at 194.8
ppm, consistent with HXe dissolved in oxygenated blood, steadily grows in
amplitude with T1,RF. It is interesting to note that additional
resonances corresponding to HXe dissolved in surrounding structures can be seen
at 190 – 193 ppm at a T1,RF of 14.6 s. While the spectra in the blue
ROI show similar behavior across T1,RFs, the most prominent peak at
T1,RF = 14.6 s appears to be at 196.2 ppm, consistent with HXe
dissolved in deoxygenated blood. The presence and temporal evolution of this
peak is most likely explained by real-time deoxygenation of blood within the
region coincident with the tumor, or by an influx of deoxygenated blood from
the venous system to that region. Since these images were acquired without
anterior/posterior phase encoding, localization of the spectra in that
direction was not possible.Conclusion
In
this study, we demonstrated a technique for visualizing and distinguishing HXe
dissolved in oxygenated and deoxygenated blood, showing its utility by
measuring the time evolution of blood deoxygenation within a tumorous region of
the lung. Future studies using this technique will focus on acquiring 3D
images, rather than 2D projections, to more accurately localize signal
contributions to specific anatomical compartments; these studies will also
demonstrate this technique’s utility for investigating disease models
characterized by alterations in regional blood oxygenation.Acknowledgements
No acknowledgement found.References
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