Ziyi Wang1, Leith Rankine1, Aparna Swaminathan1, Elianna A Bier1, Matthew P Thorpe2, Robert Tighe1, Yuh Chin Huang1, Sudarshan Rajagopal1, and Bastiaan Driehuys1
1Duke University, Durham, NC, United States, 2Mayo Clinic, Rochester, MN, United States
Synopsis
Hyperpolarized
129Xe gas exchange (GX) MR imaging of pulmonary ventilation, barrier
uptake and red blood cell (RBC) transfer has shown sensitivity to a wide range
of pathology. However, the physiological interpretation of regional RBC
transfer defects is not yet fully established and its connection to conventional
measures has yet to be studied in a broad range of pathology. Here we evaluate
the extent to which 129Xe RBC transfer reflects local perfusion, by
testing its spatial correlation to 99mTc scintigraphy and propose a
generalized model connecting 129Xe gas exchange metrics to the
membrane and capillary blood volume components of DLCO.
Introduction
Hyperpolarized
129Xe MRI has emerged as a powerful means to image pulmonary gas
exchange (GX), with its ability to provide 3D non-invasive mapping of
ventilation, barrier uptake and red blood cell (RBC) transfer1. Prior work
has shown 129Xe RBC transfer to be sensitive to a broad range of
pathology2. Initial application to healthy
and IPF subjects suggested the ratio of RBC:barrier correlates strongly with the
clinical measure of gas exchange — DLCO3. However, the physiological
interpretation of regional RBC transfer remains to be established. Moreover,
the simple RBC-barrier ratio does not account for factors such as emphysematous
loss of membrane conductance or accessible alveolar volume VA. Thus, we sought
to develop a comprehensive means to interpret 129Xe MRI across a broad range of
pathology. First, we evaluate the extent to which 129Xe RBC transfer imaging
reflects local perfusion by testing its spatial correlation to 99mTc
scintigraphy. Second, we propose a generalized model that uses 129Xe
GX MRI to reveal both the membrane and capillary blood volume conductance
contributions to the transfer coefficient KCO. We then use the ventilation
images to estimate accessible alveolar volume VA, and thereby
calculate the diffusing capacity DLCO.Methods
We analyzed 17
patients who had 99mTc scintigraphy within 9 months of 129Xe
MRI: 2 with chronic obstructive pulmonary disease (COPD), 6 chronic
thromboembolic pulmonary hypertension (CTEPH), 5 pulmonary arterial
hypertension (PAH), 1 left heart failure (LHF) and 3 with unknown dyspnea. 129Xe
MRI produced 3D maps of ventilation, barrier uptake and RBC transfer. RBC
images were rendered into conventional planar projections used for 99mTc
perfusion, by applying attenuation from lung parenchyma and body tissues. The averaged
coronal RBC projection was quantitatively compared to the geometric means of
the anterior and posterior 99mTc scans using 6-zone analysis. This framework
reports the functional contributions of each zone and allows calculation of a Pearson
correlation coefficient (R2) between modalities as well as Bland-Altman
plots to evaluate the limits of agreement (95% confidence intervals) for each
zone.
A generalized model to estimate DLCO from 129Xe
MRI was developed based on 95 subjects who had DLCO testing and high-quality 129Xe
MRI available. This included: 17 healthy, 21 COPD, 13 IPF, 29 nonspecific
interstitial pneumonia (NSIP), 6 LHF, and 9 PAH. Using the framework of
Roughton and Forster4 (Figure 1), we propose that image-derived mean
values of 129Xe barrier uptake and RBC transfer reflect the membrane conductance
DM and capillary blood volume Vc respectively. Therefore, KCO can be represented as KCO = (α*BarREL-1+β*RBCREL-1)-1
, where α and β are coefficients. BarREL and RBCREL are calculated by dividing the
patient’s mean value by that of the healthy reference cohort. Specifically, the
inverse of BarREL is used when it
exceeds unity, as in patients with interstitial lung diease3, allowing it to convey
both alveolar surface area and membrane thickness aspects of DM.
Image-derived DLCO is then calculated with VA estimated from the ventilation
volume VV using VA = γ*VV. Results
Figure 2 (left)
shows 99mTc and 129Xe-RBC projections in a PAH patient
and a CTEPH patient. The two modalities agreed well in the PAH patient. In
contrast, the CTEPH patient showed absent lobes on the perfusion scintigraphy,
that nonetheless exhibit signal on 129Xe projections. Over the
entire cohort, the two modalities demonstrated strong correlation (R2=0.84±0.14),
while individual zones exhibited negligible bias between modalities (within 3%),
and limits of agreement within 10%.
The DLCO model was fit across the
entire cohort (N=95) to determine
the coefficients: α=11.2, β=14.6 mL/min/mmHg/L, and γ=1.43. Figure 3 shows a 3D surface of the image-estimated
KCO as a function of BarREL and RBCREL, compared to the
clinically measured values. The associated graphs show that image estimated VA
correlates well with the measured value (R2=0.66, p<0.001).
Combining these to generate image estimated DLCO shows a good correlation (R2=0.77,
p<0.001) with the clinical measurements.
Figure 4 shows the application of
this model to images of representative subjects. Compared to the healthy
subject, all patients exhibit diminished DLCO resulting from different combination
of reduced VA (IPF, LHF, PAH), decreased barrier uptake due to emphysema, increased
barrier uptake (IPF, LHF), and diminished RBC transfer. Discussion and Conclusion
While 99mTc
and 129Xe-RBC agree well in most cases, an explanation for the poor agreement
in CTEPH patients is proposed (Figure 2). In these patients, occlusion of the larger
pulmonary arteries reduces flow, and therefore limits delivery of 99mTc
to the capillary bed. However, if the capillary bed remains viable, it will
remain filled with blood and thereby allow 129Xe RBC transfer through
interstitial diffusion5. Thus, while well-perfused regions will show good RBC
transfer, and destruction of capillary bed will decrease both, partial occlusion
of large vessels can lead to significant mismatch between 99mTc and 129Xe-RBC
imaging. (It
is notable that DLCO can be normal in CTEPH patients5).
This
interpretation is further supported by our DLCO model, which connects to
all aspects of 129Xe MR imaging. Importantly, it suggests
that 129Xe imaging permits decomposing both the membrane conductance
and capillary blood volume aspects of gas exchange, as well as resolving it
3-dimensionally.
This effort towards establishing a
framework for interpreting 129Xe RBC transfer imaging will benefit
from further verification using well-controlled animal studies. Acknowledgements
This work was
supported by the NIH (R01-HL-105643, R01-HL-126771 and HHSN268201700001C).References
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