The ANSS event ID is ak0257ej6rvd and the event page is at https://earthquake.usgs.gov/earthquakes/eventpage/ak0257ej6rvd/executive.
2025/06/10 16:23:16 61.061 -151.240 62.4 3.5 Alaska
USGS/SLU Moment Tensor Solution ENS 2025/06/10 16:23:16.0 61.06 -151.24 62.4 3.5 Alaska Stations used: AK.BRLK AK.CAPN AK.GHO AK.L22K AK.RC01 AK.SSN AT.PMR AV.RED AV.SPCL AV.STLK Filtering commands used: cut o DIST/3.3 -40 o DIST/3.3 +50 rtr taper w 0.1 hp c 0.03 n 3 lp c 0.10 n 3 Best Fitting Double Couple Mo = 5.89e+21 dyne-cm Mw = 3.78 Z = 58 km Plane Strike Dip Rake NP1 295 55 120 NP2 70 45 55 Principal Axes: Axis Value Plunge Azimuth T 5.89e+21 65 263 N 0.00e+00 24 96 P -5.89e+21 5 4 Moment Tensor: (dyne-cm) Component Value Mxx -5.79e+21 Mxy -2.79e+20 Mxz -8.17e+20 Myy 9.71e+20 Myz -2.24e+21 Mzz 4.82e+21 ------- P ---- ----------- -------- ---------------------------- ------------------------------ ---------------------------------- ---#############-------------------- ######################---------------- ###########################------------# ##############################---------# #################################------### ############# ###################----### ############# T ####################--#### ############# ####################--#### #################################-----## ###############################-------## -###########################---------- ---####################------------- --------#######------------------- ------------------------------ ---------------------------- ---------------------- -------------- Global CMT Convention Moment Tensor: R T P 4.82e+21 -8.17e+20 2.24e+21 -8.17e+20 -5.79e+21 2.79e+20 2.24e+21 2.79e+20 9.71e+20 Details of the solution is found at http://www.eas.slu.edu/eqc/eqc_mt/MECH.NA/20250610162316/index.html |
STK = 70 DIP = 45 RAKE = 55 MW = 3.78 HS = 58.0
The NDK file is 20250610162316.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/3.3 -40 o DIST/3.3 +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 2.0 100 45 -90 3.06 0.1964 WVFGRD96 4.0 165 20 -20 3.15 0.2279 WVFGRD96 6.0 160 20 -25 3.18 0.2763 WVFGRD96 8.0 160 20 -30 3.28 0.3009 WVFGRD96 10.0 285 70 -85 3.31 0.3285 WVFGRD96 12.0 285 65 -85 3.34 0.3409 WVFGRD96 14.0 285 60 -85 3.37 0.3460 WVFGRD96 16.0 285 60 -85 3.39 0.3467 WVFGRD96 18.0 290 60 -80 3.42 0.3403 WVFGRD96 20.0 285 55 -85 3.45 0.3261 WVFGRD96 22.0 285 60 -80 3.46 0.3061 WVFGRD96 24.0 265 80 -55 3.45 0.2926 WVFGRD96 26.0 265 75 -55 3.47 0.2815 WVFGRD96 28.0 250 90 -55 3.47 0.2767 WVFGRD96 30.0 70 85 55 3.48 0.2753 WVFGRD96 32.0 75 50 55 3.53 0.2907 WVFGRD96 34.0 80 45 65 3.57 0.3219 WVFGRD96 36.0 70 45 55 3.58 0.3563 WVFGRD96 38.0 70 45 55 3.60 0.3905 WVFGRD96 40.0 75 40 60 3.69 0.4350 WVFGRD96 42.0 80 40 65 3.72 0.4502 WVFGRD96 44.0 75 40 60 3.73 0.4631 WVFGRD96 46.0 75 40 60 3.75 0.4749 WVFGRD96 48.0 70 40 55 3.76 0.4828 WVFGRD96 50.0 70 45 55 3.76 0.4884 WVFGRD96 52.0 70 45 55 3.77 0.4944 WVFGRD96 54.0 70 45 55 3.77 0.4974 WVFGRD96 56.0 70 45 55 3.78 0.4998 WVFGRD96 58.0 70 45 55 3.78 0.5010 WVFGRD96 60.0 70 45 55 3.79 0.4983 WVFGRD96 62.0 70 45 55 3.79 0.4974 WVFGRD96 64.0 70 50 55 3.80 0.4934 WVFGRD96 66.0 70 50 55 3.80 0.4906 WVFGRD96 68.0 65 50 50 3.80 0.4869 WVFGRD96 70.0 65 50 50 3.81 0.4830 WVFGRD96 72.0 65 50 50 3.81 0.4775 WVFGRD96 74.0 65 50 50 3.81 0.4712 WVFGRD96 76.0 70 45 50 3.82 0.4669 WVFGRD96 78.0 70 45 50 3.82 0.4604 WVFGRD96 80.0 70 45 50 3.83 0.4541 WVFGRD96 82.0 70 45 50 3.83 0.4474 WVFGRD96 84.0 65 40 45 3.85 0.4435 WVFGRD96 86.0 65 40 45 3.85 0.4366 WVFGRD96 88.0 65 40 45 3.85 0.4314 WVFGRD96 90.0 65 40 45 3.86 0.4256 WVFGRD96 92.0 60 45 40 3.86 0.4196 WVFGRD96 94.0 60 45 40 3.87 0.4143 WVFGRD96 96.0 65 45 45 3.86 0.4077 WVFGRD96 98.0 65 45 45 3.87 0.4021
The best solution is
WVFGRD96 58.0 70 45 55 3.78 0.5010
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/3.3 -40 o DIST/3.3 +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