The goal of this work is to evaluate novel MRI technique entitled Relaxation Along a Fictitious Field (RAFF) in the rotating frame of rank n (RAFFn, with n=4) in its ability to detect ischemia, specifically when tuning the sensitivity of RAFF4 to exchange processes of amide protons. Relaxation maps were thus measured in healthy and infarcted rats at 24h post stroke, and were compared with other conventionally used quantitative MRI modalities. RAFF4 robustly detected infarcted regions with enhanced contrast as compared to T1 relaxation and MTR asymmetry, thus offering a sensitive novel MRI marker for quantifying tissue abnormalities during ischemia.
Five male Sprague-Dawley (SD) rats (weighing 200-250g) were used for MRI experiments. A middle cerebral artery occlusion was performed as described previously (4). Animals were anaesthetized with isofluorane (3% for induction and 2% during scanning) via a vaporizer with a mixture of air. During the scanning the body temperature was maintained at 37°C with a heating pad, while respiration rate was constantly monitored using MR compatible devices.
Animals were scanned at baseline and at 24 hours post stroke on a 9.4 T Agilent MRI scanner. Images were acquired in a single slice (thickness=2mm), centred on thalamus. Chemical Exchange Saturation Transfer (CEST) measurements were acquired using a gradient-echo sequence (matrix: 64x64, TR=2.11ms, TE=1.07ms, FOV=20x20mm²) with a saturation train of Gaussian pulses at 0.6μT (n=80, pulse duration=50ms, flip angle=360°, 90% duty cycle). Saturation was applied at 71 frequency offsets between -5.0 and 5.0ppm. MTR asymmetry and APT* were generated as described previously (5).
T2 - weighted images were collected using Multiple Spin Echo (MSE) pulse sequence consisting of a 90° Sinc excitation pulse along the x axis (duration=2ms) followed by 10 Sinc refocusing pulses along the y axis (duration=1.6ms). Other parameters were as follows: TR=3s, time interval between the peaks of the pulses τ=8.33ms, slice thickness=2mm, FOV=20x20mm², matrix size=64x64.
An inversion recovery EPI sequence was used to quantify the T1 values. A global adiabatic inversion pulse (duration=2ms) was applied followed by 10 inversion times exponentially spaced from 8.1ms to 7.5s. Other parameters were as follows: TR=15s, TE=25.5ms, slice thickness=2mm, FOV=20x20mm², matrix size=64x64.
RAFF4 measurements were taken using a train of RAFF4 pulses (0, 20, 50, 100) with pulse parameters omega1=244 Hz and pulse duration Tp=4.525ms followed by a single shot spin echo EPI read out with parameters: TR=3s, TE=25.5ms, slice thickness=2mm, FOV=20x20mm², matrix size=64x64.
The simulations were conducted using full set of two-pool Bloch-McConnell equations, as described in (2). Spin populations of the pools were set to Pa=0.1 and Pb =1-Pa and tex between the pools of 10ms. Simulation of evolution of magnetization was done in Matlab by solving Bloch McConnell equations by numerical partial differential equation solver.
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2. Liimatainen T, Mangia S, Ling W, Ellermann J, Sorce DJ, Garwood M, et al. Relaxation dispersion in MRI induced by fictitious magnetic fields. J Magn Reson San Diego Calif 1997. 2011 Apr;209(2):269–76.
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5. Jin T, Wang P, Zong X, Kim S-G. MR imaging of the Amide-Proton Transfer effect and the pH-insensitive Nuclear Overhauser Effect at 9.4 T. Magn Reson Med Off J Soc Magn Reson Med Soc Magn Reson Med. 2013 Mar;69(3):760–770.