Haidong Li1, Zhiying Zhang1, Xiuchao Zhao1, Yeqing Han1, Xianping Sun1, Chaohui Ye1, and Xin Zhou1
1Key Laboratory of Magnetic Resonance in Biological Systems, State Key Laboratory of Magnetic Resonance and Atomic and Molecular Physics, National Center for Magnetic Resonance in Wuhan, Wuhan Institute of Physics and Mathematics, Chinese Academy of Sciences, Wuhan, People's Republic of China
Synopsis
In this study, the pulmonary gas-exchange
function was quantitatively evaluated globally and regionally by hyperpolarized
129Xe MRI using the method of chemical exchange saturation transfer
(CEST). A new parameter, named as pulmonary gas consumption time constant (Toc),
was proposed to characterize the gas exchange function. The parameter showed
significant difference between the COPD and healthy rats, and we believe it
will be a useful parameter in evaluating the pulmonary function.
Purpose
To quantitatively evaluate the pulmonary gas-exchange
function globally and regionally by hyperpolarized 129Xe MRI using the
method of chemical exchange saturation transfer (CEST).Methods
All the experiments were performed on a Bruker
Biospec 4.7T MRI scanner. 129Xe gas was polarized by a homebuilt
polarizer, and the available spin polarization is about 15%. 12 SD
rats weighted about 250g were used, including 6 healthy and 6 tobacco-induced COPD
rats. The pulse sequence for measuring dissolved xenon dynamics of
lung was shown in the Fig.1. The first excitation RF pulse with flip angle of α1 (less than 10 degree) was intended to
calibrate the xenon signal, and the second excitation pulse with flip angle of
90 degree was for generating xenon signal. Between the two excitation pulses, a
series of saturation pulses centered at 200 ppm (relative to the gas phase)
with duration of 1 ms were applied, in order to saturate dissolved xenon
signal. Following each saturation pulse, a spoiler gradient pulse with duration
of 1 ms was applied to destroy the residual transversal magnetism. Because of
the scanner’s limitation, a delay of 1 ms was added. To achieve hyperpolarized 129Xe
signal in the lung varied with the saturation time, the number of the
saturation pulses varied from 50 to 1000. The interval time between the first saturation
pulse and the second excitation pulse was set to a constant, which was 3000 ms
in this study, to avoid the relaxation influence in different acquisition with
varied saturation time. A new parameter, named as the global pulmonary gas
consumption time constant (Toc) was defined to quantify the speed of
gas in the alveoli diffusing into the alveolar tissue. It could be extracted by
fitting the data to the function S(t)=S0*e(-t*n/Toc). Imaging experiments utilized a fast low angle
shot pulse sequence (FLASH), and the sequence was shown in the Fig.2. The
excitation RF pulses for the imaging sequence were centered on the gas-phase
resonance. Before the data acquisition, 100 RF saturation pulses (Gauss-shaped,
1 ms duration, 90 degrees flip angle) were applied, with a 1 ms spoiler
gradient pulse and a delay of 1 ms following each pulse. These saturation
pulses were centered at either 200 ppm (CEST experiment) or at -200 ppm
(control experiment). The pulse sequence parameters for imaging included:
TR/TE, 10 ms/4 ms; flip angle, 7 degrees; FOV, 5 cm X 5 cm; matrix, 96X96; no
slice selection.Result and discussion
The mean consumption time constant (Toc)
in COPD and healthy rats was 0.95 ± 0.16 s and 0.63 ± 0.06 s, respectively. The
consumption time constant significantly increased (P = 0.004) in the COPD rats.
The typical consumption time constant distribution images acquired from healthy
rat and COPD rat were shown in the Fig. 3, (A) and (B) respectively. The
consumption time in the trachea was obviously higher than in the tissue in both
healthy and COPD rats, and this is most possible reason was that almost no gas
exchange occurs in the region of the trachea. Compared with the healthy rat,
the consumption time distribution increased in COPD rat lung parenchyma
significantly. Furthermore, the consumption time constant distribution in COPD
rat (D) shifted toward higher values compared to that in the healthy one (C).
This is mostly because the smoking exposure changed the thickness and the
diffusion capacity of alveolar barrier in tobacco-induced COPD rats.Conclusion
In
this study, the pulmonary gas-exchange function was quantitatively evaluated
globally and regionally using chemical exchange saturation transfer (CEST), and
a new parameter, named as pulmonary gas consumption time constant (Toc),
was proposed to characterize the gas exchange function. The parameter showed
significant difference between the COPD and healthy rats, and we believe it
will be a useful parameter in evaluating the pulmonary function. Acknowledgements
We acknowledge the support by the National
Natural Science Foundation of China (81227902, 81625011, 81601491) and National
Program for Support of Eminent Professionals (National Program for Support of
Top-notch Young Professionals).References
1.Li H, Zhang Z, Zhao X, et al. Quantitative
Evaluation of Radiation-Induced Lung Injury with Hyperpolarized Xenon Magnetic
Resonance. Magnet Reson Med, 2016, Vol 76(2),
408-416.
2.Zhang Z, Guan Y, Li H, et al. Quantitative
Comparison of Lung Physiological Parameters in Single and Multiple Breathhold
with Hyperpolarized Xenon Magnetic Resonance. Biomedical Physics &
Engineering Express, 2016, Vol 2(5), 055013.