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We first investigated the theoretical detection limits of PDQ using a simulated dipole field.
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This was verified using a simulated exercise.
For middle sources in Figure 5(b), the estimated dipole sources are lateral to the simulated dipole sources when using the BSCR larger than the correct value and the estimated dipole sources are mesial to the simulated dipole sources when using the BSCR smaller than the correct value.
The estimated dipole sources are localized below the simulated dipole sources when the used BSCR is smaller than the correct BSCR for shallow sources.
These results are consistent with the observations of Figure 4. On the other hand, the estimated dipole sources are localized above the simulated dipole sources when the used BSCR is larger than the correct BSCR, as indicated in Figure 5(a).
The dipole estimated based on a single CPD component is located in between the simulated dipole sources.
We generated simulated dipole emission patterns for normally distributed polar and azimuthal lab-coordinate dipole orientation angles (θp,φp).
The estimated dipole sources were compared with the simulated dipole sources to evaluate EEG source localization accuracy.
The trajectory previously used has been simulated using an assumed dipole that differs from the true one.
Another technique is the correction by using a dipole model [4].
Here, we attempted to model the activity over an extended area of cortex using a single dipole source.
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