Moyoko Tomiyasu1, Yasuka Sahara1, Etsuko Mitsui1, Hiroki Tsuchiya2, Takamasa Maeda2, Nobuhiro Tomoyori3, Makoto Kawashima3, Tatsuya Higashi1, Atsushi Mizota3, Kohsuke Kudo4, and Takayuki Obata1
1Department of Molecular Imaging and Theranostics, National Institutes for Quantum Science and Technology, Ciba, Japan, 2Department of Medical Technology, National Institutes for Quantum Science and Technology, Ciba, Japan, 3Department of ophthalmology, Teikyo University, Tokyo, Japan, 4Department of Diagnostic and Interventional Radiology, Hokkaido University Hospital, Sapporo, Japan
Synopsis
We observed the movement of 17O-labelled
water (H217O) in the eyes of three volunteers using
dynamic T2W 1H-MRI (3T). After a drop of H217O
saline in the right eye, the signal intensity in the right anterior chamber decreased,
reaching a minimum at 7–9 min, and then gradually recovered to close to that seen
before the eye drop, by about 40 min. Signal decrease and recovery was also
observed in the posterior chamber, but not in the vitreous body. These results show that H217O drops flow
smoothly into the human anterior chamber and flow out slowly.
Introduction
Abnormalities in the water flow in the anterior chamber cause eye diseases such as glaucoma [1]. Gadolinium, as an MRI contrast agent, does not readily pass through the blood-retinal barrier or the blood-aqueous barrier of capillaries that supply water to the eye; therefore, it is difficult to visualize the flow of ocular aqueous humor. The protons in H217O have various Larmor precession frequencies due to the scalar coupling with 17O [2]. The chemical exchange of protons between H217O and H216O shortens the T2 of the water protons. As a result, the T2WI signal intensity in the region with H217O is lower than that with only H216O. Recently, an in vivo experiment on the human brain using dynamic T2W 1H-MRI of H217O was reported [3]. Our study using eye drops of H217O saline was designed to observe the distribution of H217O in the eye and its flow into and out of the anterior chamber using dynamic T2W 1H-MRI.Methods
Three healthy
female volunteers (20–31
years old) participated in our study. The parameters of the dynamic T2W
1H-MRI
(3T, Siemens, Erlangen, Germany) were as follows: a half-Fourier, single-shot,
turbo-spin echo sequence [4],
TR/TE, 3000/444 msec; field-of-view (FOV), 180×180 mm; slice thickness, 3
mm; and matrix, 320×320
pixels, reconstructed to 640×640. The total scan time was
42 min, and each subject performed the following sequence of actions: 1-min,
rest (Eyes_closed); 1-min, stare at a single point to avoid eye movement
(Eyes_open); 1-min, applied eye drops to her right eye with 10 mol% H
217O
saline (0.92–1.43 mL; TAIYO NIPPON SANSO, Tokyo, Japan); 9-min, Eyes_open;
5-min, Eyes_closed; 10-min, Eyes_open; 5-min, Eyes_closed;
10-min, Eyes_open.
In-house software developed in MATLAB
(MathWorks, MA, USA) was used for the data analysis. Images obtained during Eyes_closed
periods and those with motion artifacts were not used in the analysis. Three
averaged images were created from 10 consecutive images obtained at the
following time points: i) just after the application of the eye drop, ii) when the
signal intensity was the lowest, and iii) during the signal recovery; then the
image obtained prior to the eye drops was subtracted from each of them.
To obtain the normalized signal intensity
of the right anterior chamber (nAC), in a single image, the right and left
anterior chambers were manually selected as regions-of-interest (ROIs), each of
size 1.66 mm
2 (7×3 pixels), and the right-ROI signal intensity was
divided by that of the left. For each of all dynamic images, the ROIs were set
at the same position as the two selected ROIs. A linear relationship between H
217O
concentration and the relaxation rate change (ΔR
2) of MR signal
intensity has been reported [5,
6].
The ΔR
2 of nAC at time t was calculated using the following equation:
- ΔR2(t) = [−ln{nAC(t)/nAC(0)}]/TE, (1)
where nAC(0) is the
signal intensity before the eye drop. Then, a biexponential curve was fitted to
the time variation of ΔR
2:
- ΔR2(t) =
A{−exp(−Bt) + exp(−Ct)}, (2)
where A is a constant
coefficient, and B and C are the inflow and outflow constants, respectively.
Results
The
variations in nAC across time were similar for all subjects: the signal intensity
decreased after the eye drop, to a minimum at 7–9 min, and then began to
recover, reaching a value close to nAC(0) at 40 min. The subtracted images
showed decreases in signal intensity in the anterior and posterior chambers but
not in the vitreous body (Fig. 1). The inflow and outflow constants for the three
subjects ranged 0.195–0.326 min-1 and 0.026–0.240 min-1,
respectively (Fig. 2).Discussion
The time changes of
nAC and the inflow and outflow constants were similar for the three subjects. These
results show that the H217O saline eye drops flow smoothly
into the anterior chamber and flow slowly out again, as can be observed using dynamic
T2W 1H-MRI.
There have been no reports of H217O
being administered to human eyes in vivo, but there are a few reports in
animals [6,
7].
Kwong et al. administered H217O to the rabbit eye [6].
Similar observations in rabbit eyes were reported by Obata et al. in 2H-MRI
with D2O [8].
With the application of eye drops to the rabbit eye in those studies [6,
8],
outflow of H217O and of D2O from the anterior
chamber gave similar results, with a constant of about 0.1 min-1. Our
outflow constants ranged from 0.026 to 0.240 min-1, which include
the above value, but with such a large range in our values, 0.1 cannot clearly
be considered ‘similar’. Our large range may indicate that there are large
individual differences in humans, including the instability due to the very
long scan time. For T2WI, the D2O study reported signal changes in
the vitreous body [8], therefore in our study, the possibility of signal changes at the noise level due to
the flow of H217O into the vitreous body cannot be ruled
out.Conclusions
Our results using dynamic T2W 1H-MRI
showed that H217O saline eye drops were distributed in the
human anterior and posterior chambers and smoothly flowed into, and slowly out of,
the anterior chamber. Further measurements on healthy subjects are needed to
confirm differences in age and other factors.Acknowledgements
This work was supported by a
Grant-in-Aid (Public/Private R&D Investment Strategic Expansion PrograM:
PRISM) from the Cabinet Office, Japan.
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