Diffusional kurtosis imaging (DKI) is a significant extension of diffusion tensor imaging, providing sensitive biomarkers to diseases at the cost of lengthy acquisition and post-processing time. Fast DKI method operating with kurtosis tensor and based on axially symmetric approximation was then proposed to overcome the disadvantage. To explore the clinical utility of fast DKI, a Monte Calo simulation was conducted on a tissue model to validate the sensitivity of fast kurtosis measurements to four microstructural changes. The results suggest that fast DKI method is reliable with reduced scan time but considerable sensitivity to microstructural Changes frequently occurred in neurological diseases.
Conventional DKI (CDKI) method uses two b value and 30 directions, with a total of 61 diffusion weighted images including b0 image, to fit the signal equation (1) in Table 1 to get the 21 unknowns of diffusion tensor and kurtosis tensor, enabling the estimation of mean and directional kurtosis defined in (2) of Table 1. Fast DKI (FDKI) makes use of mathematically more convenient kurtosis tensor $$$W(\widehat{n})$$$ to define fast kurtosis parameters in line (4) in Table 1. The new definitions enable direct computation of $$$\overline{W}$$$ from diffusion signal along nine determined directions, and $$$W_{\perp}$$$ from 4 directions, $$$W_\parallel$$$ from 1 direction if the principle diffusion direction is known. Even though only in regions like spinal cord or peripheral nerve the principal direction of images is a priori knowledge, approximating axial symmetry of diffusion and kurtosis tensor allows the new signal equation be written as (3) in Table1, reducing the unknowns to only 8, thus enabling a fast determination of DKI parameters by nonlinear fitting to the 19 measurements acquired with 199 protocol 4.
To explore the validity of sensitivity of fast kurtosis parameters to tissue microstructural changes and compare it to the conventional ones, we adopted a tissue model containing axons, glial cells, and extra-axonal space 6. The axon and the glial cell were modeled by cylinder and ellipsoid respectively and a hexagonal shape was chosen as the basic unit for its more efficient use of space as shown in Figure 1. Four microstructural changes leading to certain pathologies frequently appeared in TBI, stroke, glioma or neurodegenerative diseases were simulated as shown in Table 2. 6-9 Simulations contain a group of 1.2×105 particles. Axon radius/glial cell short axis is 1/0.7μm resulting to axon/glial fraction of 40.31% /14.75% at normal state. Extra-axonal diffusivity is 2μm2/ms and glial membrane permeability is 0.001cm/s. The diffusion process was discretized by separating the diffusion time D (50ms) into T (10000) steps, and diffusion-weighted signal was synthesized following the time evolution of the pulsed gradient spin echo sequence. Signals of b=1000, 2600s/mm2 from 9 directions for FDKI estimation and 30 equally spaced directions for CDKI are simulated. A nonlinear fit was used for both fast and conventional DKI.
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