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Cited by 51 publications
(60 citation statements)
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“…[231] T 1 values for spins of hydrocarbons are typically much shorter (~ 1 s) than that of 129 Xe, limiting the transport time of fluid from the sample to the detector; however, if the sample coil and the detection coil are close enough and the flow rate is sufficiently high, the experiments are feasible. Because the gyromagnetic ratio and the natural abundance of 1 H is much higher than for 129 Xe, the sensitivity in PHIP experiments may be significantly higher.…”
Section: Remote-detection Mri Of Hyperpolarized Gasesmentioning
confidence: 99%
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“…[231] T 1 values for spins of hydrocarbons are typically much shorter (~ 1 s) than that of 129 Xe, limiting the transport time of fluid from the sample to the detector; however, if the sample coil and the detection coil are close enough and the flow rate is sufficiently high, the experiments are feasible. Because the gyromagnetic ratio and the natural abundance of 1 H is much higher than for 129 Xe, the sensitivity in PHIP experiments may be significantly higher.…”
Section: Remote-detection Mri Of Hyperpolarized Gasesmentioning
confidence: 99%
“…[231a] Overall, the combined sensitivity gain provided by the RD scheme and PHIP was 48,000-fold, and the experiments turned out to be one to two orders of magnitude more sensitive than the corresponding RD experiments with HP Xe. Comparison of the TOF images of a gas and a liquid (Figures 15b and 15c) nicely depicts different flow behavior of these phases; laminar flow of a liquid translates the encoded liquid molecules over a large distance (Figure 15c), whereas for a gas the three orders of magnitude faster diffusion causes efficient mixing of the flow lamellas, leading to a significantly less dispersed, plug-like flow behavior (Figure 15b).…”
Section: Remote-detection Mri Of Hyperpolarized Gasesmentioning
confidence: 99%
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