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. 2015 Sep 22;10(9):e0138325. doi: 10.1371/journal.pone.0138325

Fig 2. Background Filter Performance.

Fig 2

Field shifts are calculated based on the numerical susceptibility phantoms (first column) by dipole convolution and are falsified by artificial harmonic background inhomogeneities (second column). The top row shows a homogeneous phantom, the bottom row includes strong susceptibility spikes. SPHINX, DIPF and MUBAFIRE (Local) are applied to the cases. Red arrows indicate artefacts.