Robin A. Damion1,2,3, Daniel J. Cocking3,4, Brett Haywood3,4, Matthew S. Brook2,5,6, Paul L. Greenhaff2,5,6, Philip J. Atherton1,2,5, Dorothee P. Auer1,2,3, and Richard Bowtell2,3,4
1School of Medicine, University of Nottingham, Nottingham, United Kingdom, 2NIHR Nottingham Biomedical Research Centre/Nottingham Clinical Research Facilities, University of Nottingham, Nottingham, United Kingdom, 3Sir Peter Mansfield Imaging Centre, University of Nottingham, Nottingham, United Kingdom, 4School of Physics & Astronomy, University of Nottingham, Nottingham, United Kingdom, 5MRC-Versus Arthritis Centre for Musculoskeletal Ageing Research, University of Nottingham, Nottingham, United Kingdom, 6School of Life Sciences, University of Nottingham, Nottingham, United Kingdom
Synopsis
Deuterium
spectra of the human calf were obtained at natural abundance, at 3 T field
strength. Two peaks with a chemical shift separation of 3.5 ppm were observed,
corresponding to water and lipids, and their relaxation times T1 and T2* were measured using a transceive surface coil.
Utilising the complex data to fit spectral lines, including independent phases
for each peak, and fitting the complex inversion-recovery data enabled measurements
of T1 which could be
frustrated by inversion-time-dependent phases caused by RF imperfections. The
results indicate that such measurements in humans are possible despite the low
natural abundance of 2H.
Introduction
Use of deuterium oxide D2O
as a tracer allows simultaneous measurement of the turnover of multiple
substrate pools in free-living humans in short and long term studies1. Deuterium magnetic resonance allows in vivo
measurement of uptake and metabolization of D2O. In such studies,
spectra often display two dominant peaks; water (HDO) and a peak appearing at a
chemical shift of approximately 2.7 – 3.8 ppm lower2 – 6. The reported position of this second peak varies
within the literature and might be dependent on the metabolic context of the
research. Here, as a precursor to tracer studies we have explored the deuterium
spectrum obtained from the lower leg at natural abundance, characterising the T1 and T2* relaxation times of the two spectral lines and
demonstrating that measurements are feasible at 3 T magnetic field strength on
a clinical scanner using a transceive, surface RF coil.Methods
Non-localised inversion-recovery
measurements were performed on the calf of four human volunteers, using an
in-house-built deuterium surface coil (planar, 12.5 cm approximate diameter)
resonating at 19.6 MHz, interfaced to a Philips Achieva 3T imaging system. The
coil produced a field of approximately 40 μT
at the calf surface. Inversion was achieved by a 900 Hz bandwidth adiabatic
pulse, followed by a period, τ,
before a non-selective RF pulse of 90°
nominal flip-angle was applied. Further experimental details are given in
Figure 3.
Data were analysed using code
written in MATLAB (MathWorks, Natick, USA). Spectra acquired with an
inhomogeneous surface coil over a large volume can possess peaks with different
phases due to the averaging of various RF factors over a spatial concentration
distribution which is different for the molecules producing the spectral peaks.
Therefore, a global zeroth-order phase-correction cannot be applied. Instead, the
complex spectra were fitted to a sum of two complex Lorentzian lineshape
functions employing independent phases for each spectral peak, as well as
amplitude, frequency, and R2*.
The inappropriateness of a simple phase-correction and the fact that the phases
are functions of inversion time (other than the usual phase-shift at the
null-point) mean that the inversion-recovery curve also needs to be analysed as
a complex function, as
$$M(τ)=α-β \exp \left( -\frac{τ}{T_1}\right) + (β-α) \exp\left( -\frac{T_{\mathrm R}}{T_1}\right), \quad α,β\in\mathbb{C}, \quad T_1\in\mathbb{R}, \qquad\qquad\qquad\qquad (1)$$
where $$$M(τ)$$$ is the complex magnetization
(determined by the spectral amplitude and phase). Results
Figure 2 shows a typical spectrum
of the natural abundance deuterium from the calf. Two peaks are clearly visible:
a water peak (HDO) and a peak at 3.5 ppm lower. After correcting for applied line-broadening,
mean T2* values were
obtained for HDO of 8.2 ±
1.6 ms, and 14.0 ± 2.5
ms for lipids (n=4, see Table 1).
Figure 3 shows a set of spectra
acquired during an inversion-recovery experiment. All spectra were globally
shifted in reference to the spectrum of longest inversion time. Figure 4 shows
the complex spectral amplitudes and their fitted lines according to equation 1,
for each of the two peaks (HDO and lipids). Mean T1 values were found to be 199 ± 34 ms for HDO and 56 ± 10 ms for lipids (n=4, see Table 1).Discussion
From our measurements of the
lipid signal’s 3.55 ppm chemical shift, it most likely originates predominantly
from deuterium in methylene groups (-CH2-) of fatty acids and
triglycerides, consistent with signals observed in proton MRS7, in agreement
with most previous in vivo 2H measurements. In studies that
administered D2O to normal, obese, and diabetic mice, water and a second
peak—assumed to be CHD groups from adipose tissues—were observed2,3, and the position of the CHD peak was
in the approximate range 3.4 ±
0.4 ppm below the water resonance. Similarly, experiments on rats produced a lipid
signal at approximately 3.4 ppm below the water peak4. In contrast, during experiments on the
hind limbs of mice with tumour xenografts5,6,
an HDO peak was observed along with a second peak at 2.8 ppm below the water
position. In this case, it was suggested5
that this peak arose from cholesterol (or esters of), which is actively
synthesised in many tumour cells.
Previous deuterium T1 measurements in muscle water
produced values of 130 ±
7 ms (mouse, 9.2 MHz, 25°C)8 and 160 ±
2.4 ms (rat, 13.7 MHz, ex vivo)9.
Our measured values are higher, possibly due to the higher field strength and
in vivo temperature. A previous measurement of the “CHD group” found T1 = 34 ± 4 ms (mouse abdomen, 30.7
MHz, in vivo)2, which is
smaller than the value measured here. Our longer value could be a consequence
of reduced accuracy caused by incomplete inversion of the lipid magnetization
because of its short relaxation time10.Conclusions
Water (HDO) and lipids (probably
triglycerides) were identified in the in vivo spectra from the human calf.
Relaxation times T1 and T2* were also measured and
were consistent with literature values. Despite poor signal-to-noise ratio at
natural abundance and the use of a surface coil for transceive, it was shown
that such measurements are possible in a reasonable time period (approximately
30 minutes), suggesting that tracer-based metabolic studies of, e.g.,
triglyceride synthesis and turnover are possible in humans, and in such
experimental conditions. Acknowledgements
This research was funded by the NIHR Nottingham Biomedical
Research Centre. The views expressed are those of the authors and not
necessarily those of the NHS, the NIHR or the Department of Health and Social
Care. DJC’s Ph.D. studies are funded by the Precision Imaging Beacon at the
University of Nottingham.References
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