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. Author manuscript; available in PMC: 2014 Feb 1.
Published in final edited form as: J Magn Reson Imaging. 2013 Feb;37(2):313–331. doi: 10.1002/jmri.23844

Figure 12.

Figure 12

XTC: Xenon polarization transfer contrast. Following inhalation of hyperpolarized gas, a low-flip-angle, gradient-echo image of gas-phase 129Xe is acquired (left). Next, image contrast reflecting the degree of gas exchange between the airspaces and tissue/blood is generated by applying a series of high-flip-angle RF pulses (green arrows in plots) at the frequency corresponding to the dissolved-phase compartments. During the delay between applications of these contrast-generating high-flip-angle RF pulses, exchange of xenon atoms between the airspaces and tissue/blood causes the gas-phase longitudinal magnetization to decrease (plot on right, blue curve) by an amount proportional to the degree of exchange. Finally, a second low-flip-angle, gradient-echo image of gas-phase 129Xe is acquired (right). Analysis of the changes in signal intensity between the first and second images provides a regional map (top) reflecting the degree of gas exchange that occurred during the delay between contrast-generating RF pulses. For clarity, the dissolved-phase peaks (plot on left) and associated plots of longitudinal magnetization (plot on right) are shown several times larger than actual values.