The ANSS event ID is ak025d59j5t5 and the event page is at https://earthquake.usgs.gov/earthquakes/eventpage/ak025d59j5t5/executive.
2025/10/13 16:51:16 60.198 -153.707 188.4 4.1 Alaska
USGS/SLU Moment Tensor Solution
ENS 2025/10/13 16:51:16.0 60.20 -153.71 188.4 4.1 Alaska
Stations used:
AK.BRLK AK.CAST AK.L17K AK.L19K AK.N15K AK.N18K AK.O14K
AK.O18K AK.O19K AK.PPLA AK.SWD AV.RED II.KDAK
Filtering commands used:
cut o DIST/4.5 -10 o DIST/4.5 +60
rtr
taper w 0.1
hp c 0.03 n 3
lp c 0.10 n 3
Best Fitting Double Couple
Mo = 2.11e+22 dyne-cm
Mw = 4.15
Z = 188 km
Plane Strike Dip Rake
NP1 355 75 45
NP2 250 47 159
Principal Axes:
Axis Value Plunge Azimuth
T 2.11e+22 42 223
N 0.00e+00 43 9
P -2.11e+22 17 117
Moment Tensor: (dyne-cm)
Component Value
Mxx 2.45e+21
Mxy 1.36e+22
Mxz -4.98e+21
Myy -9.92e+21
Myz -1.26e+22
Mzz 7.47e+21
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-#######################----------------
-######### ###########---------- ---
######### T ###########---------- P --
######## ###########---------- -
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Global CMT Convention Moment Tensor:
R T P
7.47e+21 -4.98e+21 1.26e+22
-4.98e+21 2.45e+21 -1.36e+22
1.26e+22 -1.36e+22 -9.92e+21
Details of the solution is found at
http://www.eas.slu.edu/eqc/eqc_mt/MECH.NA/20251013165116/index.html
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STK = 355
DIP = 75
RAKE = 45
MW = 4.15
HS = 188.0
The NDK file is 20251013165116.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/4.5 -10 o DIST/4.5 +60 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 120.0 35 45 50 3.99 0.2005
WVFGRD96 122.0 35 45 50 4.00 0.2040
WVFGRD96 124.0 20 55 45 4.00 0.2148
WVFGRD96 126.0 20 55 50 4.00 0.2295
WVFGRD96 128.0 15 60 45 4.01 0.2474
WVFGRD96 130.0 15 60 50 4.04 0.3033
WVFGRD96 132.0 5 65 50 4.05 0.3593
WVFGRD96 134.0 5 65 55 4.07 0.4062
WVFGRD96 136.0 0 70 50 4.08 0.4501
WVFGRD96 138.0 -5 75 45 4.09 0.4808
WVFGRD96 140.0 -5 75 45 4.10 0.5030
WVFGRD96 142.0 -5 75 45 4.11 0.5121
WVFGRD96 144.0 -5 75 45 4.11 0.5143
WVFGRD96 146.0 355 75 45 4.11 0.5175
WVFGRD96 148.0 355 75 45 4.11 0.5189
WVFGRD96 150.0 355 75 45 4.12 0.5216
WVFGRD96 152.0 355 75 45 4.12 0.5239
WVFGRD96 154.0 355 75 45 4.12 0.5250
WVFGRD96 156.0 355 75 45 4.12 0.5256
WVFGRD96 158.0 355 75 45 4.12 0.5268
WVFGRD96 160.0 355 75 45 4.12 0.5276
WVFGRD96 162.0 355 75 45 4.13 0.5265
WVFGRD96 164.0 -5 75 45 4.13 0.5289
WVFGRD96 166.0 355 75 45 4.13 0.5295
WVFGRD96 168.0 355 75 45 4.13 0.5291
WVFGRD96 170.0 -5 75 45 4.13 0.5306
WVFGRD96 172.0 -5 75 45 4.13 0.5310
WVFGRD96 174.0 -5 75 45 4.13 0.5303
WVFGRD96 176.0 -5 75 45 4.14 0.5311
WVFGRD96 178.0 355 75 45 4.14 0.5310
WVFGRD96 180.0 355 75 45 4.14 0.5310
WVFGRD96 182.0 355 75 45 4.14 0.5318
WVFGRD96 184.0 355 75 45 4.14 0.5319
WVFGRD96 186.0 355 75 45 4.14 0.5311
WVFGRD96 188.0 355 75 45 4.15 0.5321
WVFGRD96 190.0 355 75 45 4.15 0.5312
WVFGRD96 192.0 355 75 45 4.15 0.5314
WVFGRD96 194.0 355 75 45 4.15 0.5300
WVFGRD96 196.0 355 75 45 4.15 0.5310
WVFGRD96 198.0 355 75 45 4.15 0.5293
The best solution is
WVFGRD96 188.0 355 75 45 4.15 0.5321
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/4.5 -10 o DIST/4.5 +60 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