Simultaneous Measurement of CEST and $$$T_1$$$ using Model-based Multi-Pool-Lorentzian Look-Locker Reconstruction
Motivation: Conventional quantitative CEST experiments require the additional determination of $$$T_1$$$. CEST sequences include $$$T_1$$$ relaxation periods that can be exploited to estimate $$$T_1$$$ simultaneously to the CEST parameters. Goal(s): The development of a technique for efficient simultaneous quantification of CEST contrast and $$$T_1$$$. Approach: Integration of a FLASH acquisition train after conventional CEST saturations. Simultaneous CEST contrast and $$$T_1$$$ fitting is achieved by extending the Lorentzian model of the CEST spectrum with a Look-Locker model for the FLASH readout. Results: The proof-of-concept was implemented, and first results are demonstrated in a two pools phantom and a four pool in vivo study. Impact: The presented technique enables calculating $$$T_1$$$ corrected quantitative CEST results from one measurement. This simplifies the application of the apparent exchange-dependent relaxation ($$$MTR_{AREX}$$$), the quasi-steady-state$$$\;$$$contrast and other CEST metrics, which require a $$$T_1$$$ map, making them more accessible.
Authors
- Markus Huemer (ORCID: https://orcid.org/0009-0004-9095-2626)
- Rudolf Stollberger (ORCID: https://orcid.org/0000-0002-4969-3878)
- Moritz Zaiß (ORCID: https://orcid.org/0000-0001-9780-3616)
- Nick Scholand (ORCID: https://orcid.org/0000-0002-8876-0236)
- Clemens Stilianu (ORCID: https://orcid.org/0009-0008-5033-9877)
- Daniel Mackner (ORCID: https://orcid.org/0009-0004-0123-6442)
Publication Details
- Journal
- Proceedings on CD-ROM - International Society for Magnetic Resonance in Medicine. Scientific Meeting and Exhibition/Proceedings of the International Society for Magnetic Resonance in Medicine, Scientific Meeting and Exhibition
- Published
- 2024-11-26
- DOI
- https://doi.org/10.58530/2024/4477
- Citations
- 1
- Primary Topic
- Medical Imaging Techniques and Applications
- Type
- article
- Field-Weighted Citation Impact
- 0.40