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由于壳层数模型设定错误,在单个时间点偶极子定位参数中存在潜在错误。

Insidious errors in dipole localization parameters at a single time-point due to model misspecification of number of shells.

作者信息

Zhang Z, Jewett D L

机构信息

Research Division, Abratech Corporation, Mill Valley, CA 94941-6610.

出版信息

Electroencephalogr Clin Neurophysiol. 1993 Jan-Feb;88(1):1-11. doi: 10.1016/0168-5597(93)90022-h.

DOI:10.1016/0168-5597(93)90022-h
PMID:7681385
Abstract

Insidious errors (unexpected and difficult-to-detect under usual conditions) were found using a single time-point dipole localization method, when two dipoles were simultaneously active and there was misspecification of the number of shells (usually intended to mimic the conductivity differences of the brain, skull, and scalp). The errors involved all dipole parameters (i.e., location, orientation, and magnitude). Potentials at 65 "electrode" locations on the surface of a 3-shell sphere were computed for dipoles of known location, orientation, and magnitude. These "maps" were then used to compute the best-least-squares-fit of the surface potentials based upon dipole parameters in a 1-shell sphere when either one or two dipoles were active. The dipole parameters were often significantly different when computed with two equal-magnitude dipoles active, compared with only one dipole, with location errors of 0-36 mm, orientation errors of 0-63 degrees, and magnitude errors of 2-98%. When the two dipole magnitudes were not the same, the errors in the computed dipole parameters were even larger. All these errors occurred when the LSE (least-square-error) was small and at or near minimum. Moreover, location errors increased as LSE decreased over iterations. These errors generally occur because the fitted dipole parameters under different potential maps do not obey the superposition law when there is shell model misspecification, which is also the reason that presently used "correction" methods cannot satisfactorily remove these errors from the analyses. This problem must be dealt with when analyzing evoked response "maps" from simultaneously active generators, if correspondence to anatomy and physiology is desired.

摘要

使用单时间点偶极子定位方法时发现了潜在的误差(在通常情况下难以检测到且出乎意料),当两个偶极子同时活跃且壳层数指定错误时(通常旨在模拟大脑、颅骨和头皮的电导率差异)。这些误差涉及所有偶极子参数(即位置、方向和大小)。针对已知位置、方向和大小的偶极子,计算了三壳球体表面65个“电极”位置处的电位。然后,当一个或两个偶极子活跃时,基于单壳球体中的偶极子参数,使用这些“图”来计算表面电位的最佳最小二乘拟合。与仅一个偶极子活跃时相比,当两个大小相等的偶极子活跃时计算得到的偶极子参数通常有显著差异,位置误差为0 - 36毫米,方向误差为0 - 63度,大小误差为2 - 98%。当两个偶极子大小不同时,计算得到的偶极子参数误差甚至更大。所有这些误差都发生在最小二乘误差(LSE)较小且处于或接近最小值时。此外,随着迭代过程中LSE的减小,位置误差会增加。这些误差通常是因为当存在壳模型指定错误时,不同电位图下拟合的偶极子参数不遵循叠加定律,这也是目前使用的“校正”方法不能令人满意地从分析中消除这些误差的原因。如果希望与解剖学和生理学相对应,在分析来自同时活跃发生器的诱发反应“图”时必须处理这个问题。

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