Abstract

Many potential clinical applications of chemical exchange saturation transfer (CEST) have been studied in recent years. However, due to various limitations such as specific absorption rate guidelines and scanner hardware constraints, most of the proposed applications have yet to be translated into routine diagnostic tools. Currently, pulsed CEST which uses multiple short pulses to perform the saturation is the only viable irradiation scheme for clinical translation. However, performing quantitative model-based analysis on pulsed CEST is time consuming because it is necessary to account for the time dependent amplitude of the saturation pulses. As a result, pulsed CEST is generally treated as continuous CEST by finding its equivalent average field or power. Nevertheless, theoretical analysis and simulations reveal that the resulting magnetization is different when the different irradiation schemes are applied. In this study, the quantification of important model parameters such as the amine proton exchange rate from a pulsed CEST experiment using quantitative model-based analyses were examined. Two model-based approaches were considered – discretized and continuous approximation to the time dependent RF irradiation pulses. The results showed that the discretized method was able to fit the experimental data substantially better than its continuous counterpart, but the smaller fitted error of the former did not translate to significantly better fit for the important model parameters. For quantification of the endogenous CEST effect, such as in amide proton transfer imaging, a model-based approach using the average power equivalent saturation can thus be used in place of the discretized approximation.

Highlights

  • Chemical exchange saturation transfer (CEST) is an MRI technique in which saturation is applied at the frequency of exchangeable labile protons with readout being performed from water protons

  • The average field (AF) approximation was a poor match to the pulsed spectrum; it underestimated the saturated magnetization across the simulated offsets

  • The z-spectrum generated using the AP approximation matched well the spectrum produced by the discretization method, except at the frequency offsets near the water center frequency (0 ppm) and chemical shift of amine protons (1.9 ppm), indicated by the green1 circles

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Summary

Introduction

Chemical exchange saturation transfer (CEST) is an MRI technique in which saturation is applied at the frequency of exchangeable labile protons with readout being performed from water protons. Through chemical exchange of saturated protons from the labile group to the unsaturated protons in the bulk water, a detectable signal reduction can be measured [1,2,3]. This mechanism provides an indirect way to detect dilute labile protons that would otherwise be undetectable due to their low concentration.

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