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Optimizing saturation time for maximum CEST contrast
Yifan Zhao1, Julius Juhyun Chung1, Tao Jin1
1Department of Radiology, University of Pittsburgh, Pittsburgh, PA 15203, USA.
Purpose:
To determine the optimal saturation time (Tsat) that maximizes the CEST contrast between a reference and a target signal, such as normal versus pathological tissues or pre- versus post-contrast conditions.
Methods:
The optimal Tsat (Tsat, opt) was determined from T1 and a single measurement of the normalized saturated signal (Ssat/S0). We evaluated the analytically derived Tsat, opt using simulation, phantom, and in vivo experiments.
Results:
Theoretical analysis showed that the Ssat/S0 measured at Tsat, opt is always higher than 0.37. When the repetition time (TR) is fixed or is very long (i.e., >5 T1), the Tsat, opt is independent of TR and can be derived from T1 and Ssat/S0 measured at any Tsat. When the steady state Ssat/S0 is 0.5 or 1/3, the Tsat, opt equals to T1 or T1/2, respectively. The analytically derived Tsat, opt were validated by simulation, phantom and in vivo experiment results, and can be extended to include multiple CEST and non-CEST effects (excluding changes in T1). The relative error of the Tsat,opt is <10-15% for typical CEST contrasts of <5%. For very large contrast (e.g., >10% of S0), more accurate estimation of Tsat, opt can be obtained from the averaged Ssat/S0 of the reference and target signals.
Conclusion:
Tsat, opt can be determined from T1 and a single measurement of the saturated signal. This approach simplifies optimization of Tsat in CEST experiments, especially when using relatively high saturation powers or resonance frequencies close to water.

