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ABSTRACT: Purpose
Previous studies have shown that diffusion of water through intrinsic susceptibility gradients produces a dispersion of the spin-lattice relaxation rate in the rotating frame (R1 ρ ) over a low range of spin-locking amplitudes (0 < ω1 < 100 Hz), whereas at higher ω1 and high magnetic fields, a second dispersion arises due to chemical exchange. Here, we separated these different effects and evaluated their contributions in tumors.Methods
Maps of R1 ρ and its changes with locking field were acquired on intracranial 9-L tumor models. The R1 ρ changes due to diffusion ( R1ρDiff ) were calculated by subtracting maps of R1 ρ at 100 Hz (R1 ρ [100 Hz]) from those at 0 Hz (R1 ρ [0 Hz]). The R1 ρ changes due to exchange ( R1ρEx ) were calculated by subtracting maps of R1 ρ at 5620 Hz (R1 ρ [5620 Hz]) from those of R1 ρ at 100 Hz (R1 ρ [100 Hz]). Measurements of vascular dimensions and spacing were performed ex vivo using 3D confocal microscopy.Results
The R1 ρ changes at low ω1 in tumors (5.24 ± 1.78 s-1 ) are substantially (p = 3.76 ) greater than those in normal tissues (1.36 ± 0.70 s-1 ), which we suggest are due to greater contributions from diffusion through susceptibility gradients. Tumor vessels were larger and spaced less closely compared with normal brain, which may be 1 factor contributing the susceptibility within 9-L tumors. The contrast between tumor and normal tissues for R1ρDiff is larger than for R1ρEx and for the apparent R2w .Conclusion
Images that are sensitive to the variations of spin-lock relaxation rates at low ω1 provide a novel form of contrast that reflects the heterogeneous nature of intrinsic variations within tumors.
SUBMITTER: Zu Z
PROVIDER: S-EPMC7558740 | biostudies-literature | 2020 May
REPOSITORIES: biostudies-literature
Magnetic resonance in medicine 20191227 5
<h4>Purpose</h4>Previous studies have shown that diffusion of water through intrinsic susceptibility gradients produces a dispersion of the spin-lattice relaxation rate in the rotating frame (R<sub>1</sub><sub>ρ</sub> ) over a low range of spin-locking amplitudes (0 < ω<sub>1</sub> < 100 Hz), whereas at higher ω<sub>1</sub> and high magnetic fields, a second dispersion arises due to chemical exchange. Here, we separated these different effects and evaluated their contributions in tumors.<h4>Meth ...[more]