Comparison of pulsed three-dimensional CEST acquisition schemes at 7 tesla: steady state versus pseudosteady state

Vitaly Khlebnikov, Nicolas Geades, DWJ Klomp, Hans Hoogduin, Penny Gowland, Olivier Mougin

Research output: Contribution to journalArticleAcademicpeer-review

1 Downloads (Pure)

Abstract

Purpose: To compare two pulsed, volumetric chemical exchange saturation transfer (CEST) acquisition schemes: steady state (SS) and pseudosteady state (PS) for the same brain coverage, spatial/spectral resolution and scan time. Methods: Both schemes were optimized for maximum sensitivity to amide proton transfer (APT) and nuclear Overhauser enhancement (NOE) effects through Bloch-McConnell simulations, and compared in terms of sensitivity to APT and NOE effects, and to transmit field inhomogeneity. Five consented healthy volunteers were scanned on a 7 Tesla Philips MR-system using the optimized protocols at three nominal B 1 amplitudes: 1 μT, 2 μT, and 3 μT. Results: Region of interest based analysis revealed that PS is more sensitive (P < 0.05) to APT and NOE effects compared with SS at low B 1 amplitudes (0.7–1.0 μT). Also, both sequences have similar dependence on the transmit field inhomogeneity. For the optimum CEST presaturation parameters (1 μT and 2 μT for APT and NOE, respectively), NOE is less sensitive to the inhomogeneity effects (15% signal to noise ratio [SNR] change for a B 1 dropout of 40%) compared with APT (35% SNR change for a B 1 dropout of 40%). Conclusion: For the same brain coverage, spatial/spectral resolution and scan time, at low power levels PS is more sensitive to the slow chemical exchange-mediated processes compared with SS. Magn Reson Med 77:2280–2287, 2017.

Original languageEnglish
Pages (from-to)2280–2287
Number of pages8
JournalMagnetic Resonance in Medicine
Volume77
Issue number6
DOIs
Publication statusPublished - Jun 2017

Keywords

  • APT
  • CEST
  • NOE
  • pseudosteady state
  • steady state
  • volumetric CEST sequence

Fingerprint

Dive into the research topics of 'Comparison of pulsed three-dimensional CEST acquisition schemes at 7 tesla: steady state versus pseudosteady state'. Together they form a unique fingerprint.

Cite this