Abstract
We consider the Bloch-Torrey operator, − Δ + i g x , that governs the time evolution of the transverse magnetization in diffusion magnetic resonance imaging (dMRI). Using the matrix formalism, we compute numerically the eigenvalues and eigenfunctions of this non-Hermitian operator for two bounded three-dimensional domains: a sphere and a capped cylinder. We study the dependence of its eigenvalues and eigenfunctions on the parameter g and on the shape of the domain (its eventual symmetries and anisotropy). In particular, we show how an eigenfunction drastically changes its shape when the associated eigenvalue crosses a branch (or exceptional) point in the spectrum. Potential implications of this behavior for dMRI are discussed.
| Original language | English |
|---|---|
| Article number | 125201 |
| Journal | Journal of Physics A: Mathematical and Theoretical |
| Volume | 57 |
| Issue number | 12 |
| DOIs | |
| Publication status | Published - 22 Mar 2024 |
Keywords
- Bloch-Torrey operator
- branch point
- diffusion-weighted NMR
- localization
- microstructure
- non-Hermitian operator
- pulsed-gradient spin-echo
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