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Published on: March 17, 2016
Field Strength-Dependent White Matter R1 and R2 Anisotropy of Phase-Cycled Balanced Steady-State Free Precession
Florian Birk1,2, Hamzeh Tesh1, Ali Aghaeifar1
1High-Field Magnetic Resonance, Max Planck Institute for Biological Cybernetics, Tübingen, Germany.
Relaxation rates (R2) and asymmetry indices (AI) in white matter (WM) show strong orientation dependence, increasing with field strength. Susceptibility effects drive R2 anisotropy at ultra-high fields, with other mechanisms contributing at lower fields.
Area of Science:
- Magnetic Resonance Imaging (MRI)
- Neuroimaging
- Biophysics
Background:
- Phase-cycled balanced steady-state free precession (pc-bSSFP) is a valuable MRI technique.
- Understanding white matter (WM) microstructure is crucial for diagnosing neurological conditions.
- Relaxation rates (R1, R2) and asymmetry indices (AI) provide insights into tissue properties.
Purpose of the Study:
- To investigate the orientation dependence of R1, R2, and AI in WM fiber tracts.
- To determine how this dependence changes with magnetic field strength (3T and 9.4T).
- To explore the underlying mechanisms, including susceptibility effects and magic angle effects.
Main Methods:
- Acquired pc-bSSFP data in the healthy human brain at 3T and 9.4T.
- Processed data using motion-insensitive rapid configuration relaxometry (MIRACLE) and frequency response analysis.
- Estimated fractional anisotropy (FA) and fiber-to-field angle (θ) from diffusion tensor imaging (DTI).
Main Results:
- R2 and AI exhibited significant orientation dependence, while R1 showed a weaker but noticeable dependence.
- Anisotropy increased systematically from 3T to 9.4T.
- Susceptibility effects were found to be the primary driver of R2 anisotropy at ultra-high fields (9.4T).
Conclusions:
- Microstructure-driven relaxation anisotropy significantly impacts pc-bSSFP relaxometry, especially R2.
- R2 anisotropy is predominantly driven by susceptibility at ultra-high fields.
- Additional mechanisms likely contribute to R2 anisotropy at lower field strengths.
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