The ANSS event ID is ak02565zajkq and the event page is at https://earthquake.usgs.gov/earthquakes/eventpage/ak02565zajkq/executive.
2025/05/14 22:30:33 61.483 -151.283 78.2 3.6 Alaska
USGS/SLU Moment Tensor Solution ENS 2025/05/14 22:30:33.0 61.48 -151.28 78.2 3.6 Alaska Stations used: AK.GHO AK.KNK AK.RC01 AK.SAW AK.SCM AK.SKN AK.SLK AK.SSN AT.PMR AV.SPCL AV.STLK Filtering commands used: cut o DIST/3.5 -40 o DIST/3.5 +50 rtr taper w 0.1 hp c 0.03 n 3 lp c 0.10 n 3 Best Fitting Double Couple Mo = 8.61e+21 dyne-cm Mw = 3.89 Z = 80 km Plane Strike Dip Rake NP1 335 73 121 NP2 90 35 30 Principal Axes: Axis Value Plunge Azimuth T 8.61e+21 51 281 N 0.00e+00 30 145 P -8.61e+21 22 41 Moment Tensor: (dyne-cm) Component Value Mxx -4.05e+21 Mxy -4.28e+21 Mxz -1.47e+21 Myy -3.74e+14 Myz -6.11e+21 Mzz 4.05e+21 -------------- ####------------------ #########------------------- ###########------------- --- ###############----------- P ----- #################---------- ------ ###################------------------- #####################------------------- ######################------------------ ########## ###########------------------ ########## T ############----------------- -######### #############---------------# -##########################--------------# --########################------------## ---########################----------### ----#######################-------#### ------####################----###### --------#################-######## ------------------------###### -----------------------##### --------------------## -------------- Global CMT Convention Moment Tensor: R T P 4.05e+21 -1.47e+21 6.11e+21 -1.47e+21 -4.05e+21 4.28e+21 6.11e+21 4.28e+21 -3.74e+14 Details of the solution is found at http://www.eas.slu.edu/eqc/eqc_mt/MECH.NA/20250514223033/index.html |
STK = 90 DIP = 35 RAKE = 30 MW = 3.89 HS = 80.0
The NDK file is 20250514223033.ndk The waveform inversion is preferred.
Given the availability of digital waveforms for determination of the moment tensor, this section documents the added processing leading to mLg, if appropriate to the region, and ML by application of the respective IASPEI formulae. As a research study, the linear distance term of the IASPEI formula for ML is adjusted to remove a linear distance trend in residuals to give a regionally defined ML. The defined ML uses horizontal component recordings, but the same procedure is applied to the vertical components since there may be some interest in vertical component ground motions. Residual plots versus distance may indicate interesting features of ground motion scaling in some distance ranges. A residual plot of the regionalized magnitude is given as a function of distance and azimuth, since data sets may transcend different wave propagation provinces.
Left: ML computed using the IASPEI formula for Horizontal components. Center: ML residuals computed using a modified IASPEI formula that accounts for path specific attenuation; the values used for the trimmed mean are indicated. The ML relation used for each figure is given at the bottom of each plot.
Right: Residuals from new relation as a function of distance and azimuth.
Left: ML computed using the IASPEI formula for Vertical components (research). Center: ML residuals computed using a modified IASPEI formula that accounts for path specific attenuation; the values used for the trimmed mean are indicated. The ML relation used for each figure is given at the bottom of each plot.
Right: Residuals from new relation as a function of distance and azimuth.
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The focal mechanism was determined using broadband seismic waveforms. The location of the event (star) and the stations used for (red) the waveform inversion are shown in the next figure.
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The program wvfgrd96 was used with good traces observed at short distance to determine the focal mechanism, depth and seismic moment. This technique requires a high quality signal and well determined velocity model for the Green's functions. To the extent that these are the quality data, this type of mechanism should be preferred over the radiation pattern technique which requires the separate step of defining the pressure and tension quadrants and the correct strike.
The observed and predicted traces are filtered using the following gsac commands:
cut o DIST/3.5 -40 o DIST/3.5 +50 rtr taper w 0.1 hp c 0.03 n 3 lp c 0.10 n 3The results of this grid search are as follow:
DEPTH STK DIP RAKE MW FIT WVFGRD96 2.0 20 60 -85 3.04 0.2200 WVFGRD96 4.0 260 25 -20 3.06 0.2510 WVFGRD96 6.0 270 30 -10 3.08 0.2932 WVFGRD96 8.0 195 80 60 3.18 0.3159 WVFGRD96 10.0 255 60 55 3.29 0.3450 WVFGRD96 12.0 260 60 60 3.33 0.3638 WVFGRD96 14.0 265 55 60 3.36 0.3712 WVFGRD96 16.0 265 55 60 3.38 0.3692 WVFGRD96 18.0 280 50 50 3.37 0.3640 WVFGRD96 20.0 280 50 50 3.39 0.3598 WVFGRD96 22.0 280 50 50 3.42 0.3520 WVFGRD96 24.0 275 45 20 3.39 0.3452 WVFGRD96 26.0 275 45 20 3.41 0.3458 WVFGRD96 28.0 275 45 15 3.43 0.3392 WVFGRD96 30.0 50 75 -25 3.49 0.3472 WVFGRD96 32.0 50 70 -15 3.51 0.3622 WVFGRD96 34.0 50 70 -10 3.54 0.3710 WVFGRD96 36.0 50 65 -15 3.55 0.3822 WVFGRD96 38.0 55 70 -5 3.58 0.3924 WVFGRD96 40.0 85 40 50 3.69 0.4122 WVFGRD96 42.0 85 40 50 3.72 0.4380 WVFGRD96 44.0 85 40 50 3.75 0.4611 WVFGRD96 46.0 85 40 50 3.76 0.4817 WVFGRD96 48.0 85 40 50 3.78 0.4981 WVFGRD96 50.0 85 40 45 3.79 0.5179 WVFGRD96 52.0 85 45 45 3.81 0.5398 WVFGRD96 54.0 85 45 45 3.82 0.5618 WVFGRD96 56.0 85 45 45 3.83 0.5787 WVFGRD96 58.0 85 45 45 3.84 0.5935 WVFGRD96 60.0 85 45 45 3.84 0.6026 WVFGRD96 62.0 85 45 45 3.85 0.6090 WVFGRD96 64.0 80 45 30 3.86 0.6193 WVFGRD96 66.0 80 45 30 3.86 0.6277 WVFGRD96 68.0 80 45 30 3.87 0.6349 WVFGRD96 70.0 85 35 25 3.87 0.6430 WVFGRD96 72.0 85 35 25 3.88 0.6515 WVFGRD96 74.0 90 35 30 3.88 0.6564 WVFGRD96 76.0 90 35 30 3.88 0.6609 WVFGRD96 78.0 90 35 30 3.88 0.6627 WVFGRD96 80.0 90 35 30 3.89 0.6653 WVFGRD96 82.0 90 35 30 3.89 0.6634 WVFGRD96 84.0 90 35 30 3.89 0.6624 WVFGRD96 86.0 90 35 30 3.90 0.6584 WVFGRD96 88.0 90 35 30 3.90 0.6558 WVFGRD96 90.0 90 35 30 3.90 0.6512 WVFGRD96 92.0 95 35 35 3.90 0.6451 WVFGRD96 94.0 95 35 35 3.90 0.6413 WVFGRD96 96.0 95 35 35 3.91 0.6346 WVFGRD96 98.0 95 35 35 3.91 0.6281
The best solution is
WVFGRD96 80.0 90 35 30 3.89 0.6653
The mechanism corresponding to the best fit is
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The best fit as a function of depth is given in the following figure:
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The comparison of the observed and predicted waveforms is given in the next figure. The red traces are the observed and the blue are the predicted. Each observed-predicted component is plotted to the same scale and peak amplitudes are indicated by the numbers to the left of each trace. A pair of numbers is given in black at the right of each predicted traces. The upper number it the time shift required for maximum correlation between the observed and predicted traces. This time shift is required because the synthetics are not computed at exactly the same distance as the observed, the velocity model used in the predictions may not be perfect and the epicentral parameters may be be off. A positive time shift indicates that the prediction is too fast and should be delayed to match the observed trace (shift to the right in this figure). A negative value indicates that the prediction is too slow. The lower number gives the percentage of variance reduction to characterize the individual goodness of fit (100% indicates a perfect fit).
The bandpass filter used in the processing and for the display was
cut o DIST/3.5 -40 o DIST/3.5 +50 rtr taper w 0.1 hp c 0.03 n 3 lp c 0.10 n 3
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Figure 3. Waveform comparison for selected depth. Red: observed; Blue - predicted. The time shift with respect to the model prediction is indicated. The percent of fit is also indicated. The time scale is relative to the first trace sample. |
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Focal mechanism sensitivity at the preferred depth. The red color indicates a very good fit to the waveforms. Each solution is plotted as a vector at a given value of strike and dip with the angle of the vector representing the rake angle, measured, with respect to the upward vertical (N) in the figure. |
A check on the assumed source location is possible by looking at the time shifts between the observed and predicted traces. The time shifts for waveform matching arise for several reasons:
Time_shift = A + B cos Azimuth + C Sin Azimuth
The time shifts for this inversion lead to the next figure:
The derived shift in origin time and epicentral coordinates are given at the bottom of the figure.
The WUS.model used for the waveform synthetic seismograms and for the surface wave eigenfunctions and dispersion is as follows (The format is in the model96 format of Computer Programs in Seismology).
MODEL.01 Model after 8 iterations ISOTROPIC KGS FLAT EARTH 1-D CONSTANT VELOCITY LINE08 LINE09 LINE10 LINE11 H(KM) VP(KM/S) VS(KM/S) RHO(GM/CC) QP QS ETAP ETAS FREFP FREFS 1.9000 3.4065 2.0089 2.2150 0.302E-02 0.679E-02 0.00 0.00 1.00 1.00 6.1000 5.5445 3.2953 2.6089 0.349E-02 0.784E-02 0.00 0.00 1.00 1.00 13.0000 6.2708 3.7396 2.7812 0.212E-02 0.476E-02 0.00 0.00 1.00 1.00 19.0000 6.4075 3.7680 2.8223 0.111E-02 0.249E-02 0.00 0.00 1.00 1.00 0.0000 7.9000 4.6200 3.2760 0.164E-10 0.370E-10 0.00 0.00 1.00 1.00