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As the subject head shapes were quite different, in some brain regions the co-registered error directions differed, thus partly cancelling each other in the mean error images.
Figure 9 shows the mean dipole source localization error directions (arrows) and magnitudes (colors), and Table 2 the median localization error magnitudes (in mm).
Thus, we calculated equivalent dipole source localization error directions and magnitudes for one four-layer reference BEM head model (S1) when the co-registered electrode montage was mistakenly tilted 5° backwards or 5° to the left (Fig. 12).
Figure 4 shows the equivalent dipole source localization error directions and magnitudes for the spherical (top row) and the four MNI-template based head models for this subject, computed from source dipole scalp projections simulated using the reference MR image-based four-layer forward head model.
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It is not reasonable for these measures to take reducing error as the only goal while ignore the error direction.
Differences between the calculation results and testing results, which including product's density, compression strength, surface evaluation, and deformation in three dimensions, are less than 10%, and have the same error direction.
To determine the impact of conduction velocity error in directions perpendicular to the fibres due to the lower conductivity, we show in Figure 5 the isosurfaces of activation times on the h = 0.02 cm mesh with p = 3.
The slightest error in direction makes it an easy four runs.
With large CCVT error correct direction estimation is a challenging task for many relaying algorithm.
The hydrophone's ability of azimuth measurement is tested with a standing-wave tube and the error of direction of arrival (DOA) estimation is within 1°.
However, because of the received noise, mutual coupling or system error, different direction finding results will be obtained when using different phase difference pairs.
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