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The observed distortions have common decay pattern for P and S waves and could be characterized by the normalized hypocentral distance kL.
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Observed distortions of the apparent P- and S-wave radiation patterns could be simply modeled by using a function of the normalized hypocentral distance, which is a product of the wave number and hypocentral distance.
Figure 3 shows the estimated CCCs as a function of the normalized hypocentral distance kL, where k is the wave number (k = 2π/λ = 2πf/V) and L is the average hypocentral distance of each distance range.
On the basis of observed normalized hypocentral distance dependency, we proposed a method for prediction of spatial distributions of maximum P- and S-wave amplitudes.
The modeled apparent radiation pattern coefficient introduced here is identical to the double-couple point source radiation pattern at small normalized hypocentral distances (
Saturation of CCC decay was found at greater normalized hypocentral distances (log kL) > 2.85), showing almost dissipation of non-isotropic source radiation effect.
This is reduced by the normalized temperature dependency factor and the normalized CO2 fertilization factor.
Each user is defined by the normalized mentioned scores.
The normalized LEE can be obtained by dividing the normalized PL integral intensity by the IQE.
The EEJ is calculated by subtracting the normalized Sq from the normalized total current.
Timescale shows time after the mainshock hypocentral time.
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