Maysam Jafar1 and Jan Weis2
1Clinical Science, Philips Healthcare, Stockholm, Sweden, 2Department of Medical Physics, Uppsala University Hospital, Uppsala, Sweden
Synopsis
Phosphorous (31P) spectra of healthy human kidney
are invaluable in studies of kidney physiology, disease and in the evaluation
of allograft viability pre and post renal transplantation. However, 31P-spectroscopy
of the kidney in-situ is challenging due to the relatively large distance
between the kidney and the surface
coil. The aim of this study
was to investigate whether it is possible to acquire 31P
spectra of normal kidney in a clinically acceptable
measurement time using a 3T MR scanner. We demonstrate that localized
phosphorous spectroscopy of normal kidney in-situ is feasible in today’s 3T
clinical MR systems.
Introduction
Phosphorus magnetic
resonance spectroscopy (31P-MRS) is a non-invasive tool for in-vivo
detection and quantification of phosphorus-containing metabolites involved in
cell membrane synthesis, cell membrane degradation and in the energy-producing
pathways necessary for cell functions 1,2. 31P-MRS of the
kidney of healthy volunteers in-situ is challenging due to the relatively large
distance (60-80 mm) between the kidney and transmit-receive 31P surface
coil. Despite this difficulty, phosphorous spectra of the normal kidney are needed
in studies of kidney physiology, disease and in the evaluation of human
allograft viability and its function pre and post renal transplantation. To the
best of our knowledge, the only reports of 31P spectra of the
healthy human kidney in-situ were published in 1988 and 1990 3,4. The main aim of this study was to investigate
the feasibility of localized 31P-MRS of normal kidney
in-situ in a clinically acceptable measurement time using
a state-of-the-art 3T MR scanner. Methods
Five healthy volunteers
participated in this study. All examinations were performed on a Philips 3T
Achieva dStream MR system. 31P spectra were acquired by a tunable
transmit-receive loop coil with a diameter of 14 cm. Single voxel spectra were
acquired using the ISIS localization sequence (TR 5000 ms, 512
scans, spectral bandwidth 3000 Hz, 2048 complex points, net acquisition time 43
min). The ISIS sequence was combined with broad-band proton decoupling and nuclear Overhauser effect
(NOE) enhancement. The whole body coil was used for imaging, decoupling and NOE
enhancement.
The acquired spectra
were fitted by Lorentzians using the AMARES algorithm (jMRUI software package 5).
No apodization of the FID was used in spectrum processing. However, a
Lorentzian apodization corresponding to 8 Hz line broadening was applied for the purpose of illustration.
The frequency axis (0 ppm) was defined by setting the phosphorylethanolamine (PE)
singlet to 6.77 ppm 6. The chemical shifts of the phosphorylcholine
(PC) and membrane phospholipids (MP) resonances with respect to the PE line were
found to be -27.92 Hz and -246.7 Hz respectively. Peak positions of inorganic
phosphate (Pi), glycerol-3-phosphorylcholine (GPC), and γ-, α-, β- adenosine triphosphate (ATP) were estimated by
AMARES. The frequency shift between GPC and glycerol-3-phosphorylethanolamine (GPE)
was fixed to 28.44 Hz. Nicotinamide adenine dinucleotide (NAD) spectral line
was placed -40.9 Hz from α-ATP 7. PE
linewidth was constrained to an interval of 5-20 Hz, Pi to 15-30 Hz, and MP to
25-40 Hz. PC linewidth was set to be equal to PE and GPE equal to
GPC. The splitting of ATP multiplets was set to 16 Hz 6. The
amplitude ratios of doublets and triplets were set to 1:1 and 1:2:1,
respectively. ATP and NAD linewidths were fixed with respect to PE using predefined ratios of 1.3, 0.9, 1.8, and 1.22 for γ-, α-, β, and NAD lines
respectively 6. The zero- and first-order phase corrections were
estimated by AMARES. The first-order correction was constrained to ±0.5 ms in the time
domain. The left kidney spectra from each volunteer were
phase and frequency corrected using the described prior knowledge and added
together.Results and discussion
A representative
voxel position is shown in Figure 1. The typical voxel size was 35 (AP) x 50 (LR) x 70 (FH) mm3. B0 shimming resulted
in a voxel water linewidth between 26 and 32 Hz. Distance between the centre of
the voxel and the surface coil was ~70±10 mm. The large depth of the kidney in human body with respect
to the surface coil combined with respiratory movement worsens SNR and the
spectral quality. To improve SNR, the
spectra of all five volunteers were added and the resulting spectrum was fitted as shown in Figure 2. The spectral intensity ratios of phosphomonoesters (PME = PE+PC),
phosphodiesters (PDE = GPE+GPC), Pi,
and (γ+ α-ATP) are shown in
Table 1. These ratios are frequently utilized in the evaluation of allograft's viability
pre and its function post renal transplantation. Total ATP spectral intensity is
preferable to these ratios but the intensity of β-ATP resonances is significantly reduced due to the non-ideal
excitation profile of the hyperbolic-secant inversion and the detection B1
pulses used in the ISIS sequence. Furthermore, B1 pulses have
limited bandwidth and their respective amplitudes drop rapidly with distance
from the transmit coil. This fast decay in amplitude results in a narrower effective
excitation bandwidth. Conclusions
We have demonstrated that localised 31P-MRS of normal kidney in-situ
is feasible in today’s 3T clinical MR scanners. Measured reference phosphorous
spectral intensity ratio of healthy kidney may prove to be beneficial in
evaluating changes in renal metabolism associated with diseases and
transplantation. Acknowledgements
We would like to thank all volunteers who took part in this study.References
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