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fractional anisotropy : ウィキペディア英語版
fractional anisotropy
Fractional anisotropy (FA) is a scalar value between zero and one that describes the degree of anisotropy of a diffusion process. A value of zero means that diffusion is isotropic, i.e. it is unrestricted (or equally restricted) in all directions. A value of one means that diffusion occurs only along one axis and is fully restricted along all other directions. FA is a measure often used in diffusion imaging where it is thought to reflect fiber density, axonal diameter, and myelination in white matter. The FA is an extension of the concept of eccentricity of conic sections in 3 dimensions, normalized to the unit range.
== Definition ==

A Diffusion Ellipsoid is completely represented by the Diffusion Tensor, D. FA is calculated from the eigenvalues (\lambda_1, \lambda_2, \lambda_3) of the diffusion tensor.〔 The eigenvectors \epsilon give the directions in which the ellipsoid has major axes, and the corresponding eigenvalues \lambda give the magnitude of the peak in that direction.
: \text = \sqrt} \frac)^2 + (\lambda_3 - \hat)^2}} = (\lambda_1 + \lambda_2 + \lambda_3)/3
An equivalent formula for FA is
: \text = \sqrt} \frac}
Note that if all the eigenvalues are equal, which happens for isotropic (spherical) diffusion, as in free water, the FA is ''0''. The FA can reach a maximum value of ''1'' (this rarely happens in real data), in which case D has only one nonzero eigenvalue and the ellipsoid reduces to a line in the direction of that eigenvector. This means that the diffusion is confined to that direction alone. Also FA can be expressed in the following form:〔
: \text = \sqrt (3-\frac)}
where R is the normalized and unitless rank-2 DT:
: \text = \frac)}

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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