The ANSS event ID is ak0237rn9mb0 and the event page is at https://earthquake.usgs.gov/earthquakes/eventpage/ak0237rn9mb0/executive.
2023/06/18 09:14:31 58.102 -154.603 84.2 5 Alaska
USGS/SLU Moment Tensor Solution
ENS 2023/06/18 09:14:31:0 58.10 -154.60 84.2 5.0 Alaska
Stations used:
AK.BRLK AK.HOM AK.M19K AK.N18K AK.O18K AK.O19K AK.P16K
AK.P17K AK.Q19K AV.ANNW AV.P19K AV.PLBL II.KDAK
Filtering commands used:
cut o DIST/3.3 -50 o DIST/3.3 +30
rtr
taper w 0.1
hp c 0.03 n 3
lp c 0.08 n 3
Best Fitting Double Couple
Mo = 3.59e+23 dyne-cm
Mw = 4.97
Z = 92 km
Plane Strike Dip Rake
NP1 85 75 45
NP2 340 47 159
Principal Axes:
Axis Value Plunge Azimuth
T 3.59e+23 42 313
N 0.00e+00 43 100
P -3.59e+23 17 207
Moment Tensor: (dyne-cm)
Component Value
Mxx -1.69e+23
Mxy -2.30e+23
Mxz 2.13e+23
Myy 4.16e+22
Myz -8.46e+22
Mzz 1.27e+23
#-------------
##########------------
################------------
###################-----------
######################------------
######## ##############-----------
######### T ###############-----------
########## ################-----------
##############################----------
###############################-----------
################################--------##
################################----######
---##########################----#########
--------------------------------########
--------------------------------########
-------------------------------#######
-----------------------------#######
----------------------------######
------ ----------------#####
----- P ----------------####
-- --------------###
--------------
Global CMT Convention Moment Tensor:
R T P
1.27e+23 2.13e+23 8.46e+22
2.13e+23 -1.69e+23 2.30e+23
8.46e+22 2.30e+23 4.16e+22
Details of the solution is found at
http://www.eas.slu.edu/eqc/eqc_mt/MECH.NA/20230618091431/index.html
|
STK = 85
DIP = 75
RAKE = 45
MW = 4.97
HS = 92.0
The NDK file is 20230618091431.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.
![]() |
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.
|
|
|
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 -50 o DIST/3.3 +30 rtr taper w 0.1 hp c 0.03 n 3 lp c 0.08 n 3The results of this grid search are as follow:
DEPTH STK DIP RAKE MW FIT
WVFGRD96 2.0 10 75 20 4.01 0.2540
WVFGRD96 4.0 195 60 35 4.13 0.2824
WVFGRD96 6.0 195 70 35 4.15 0.2966
WVFGRD96 8.0 195 70 35 4.22 0.3121
WVFGRD96 10.0 195 70 35 4.25 0.3173
WVFGRD96 12.0 195 70 30 4.27 0.3125
WVFGRD96 14.0 190 70 25 4.29 0.3031
WVFGRD96 16.0 190 75 25 4.31 0.2917
WVFGRD96 18.0 280 65 -20 4.33 0.2835
WVFGRD96 20.0 280 65 -15 4.35 0.2802
WVFGRD96 22.0 90 70 5 4.39 0.2811
WVFGRD96 24.0 90 70 5 4.41 0.2841
WVFGRD96 26.0 90 80 -15 4.43 0.2899
WVFGRD96 28.0 90 80 -15 4.45 0.2983
WVFGRD96 30.0 90 80 -15 4.47 0.3034
WVFGRD96 32.0 85 75 -15 4.50 0.3151
WVFGRD96 34.0 85 75 -15 4.53 0.3271
WVFGRD96 36.0 85 75 -10 4.56 0.3383
WVFGRD96 38.0 85 75 -10 4.60 0.3520
WVFGRD96 40.0 85 75 -15 4.66 0.3749
WVFGRD96 42.0 270 90 20 4.69 0.3836
WVFGRD96 44.0 85 80 -15 4.72 0.3977
WVFGRD96 46.0 270 90 20 4.73 0.4041
WVFGRD96 48.0 85 80 -15 4.76 0.4188
WVFGRD96 50.0 85 80 -15 4.77 0.4283
WVFGRD96 52.0 85 80 -15 4.79 0.4376
WVFGRD96 54.0 85 85 -15 4.80 0.4470
WVFGRD96 56.0 90 70 15 4.81 0.4547
WVFGRD96 58.0 90 70 15 4.83 0.4689
WVFGRD96 60.0 90 70 20 4.84 0.4841
WVFGRD96 62.0 90 70 20 4.85 0.4999
WVFGRD96 64.0 90 70 20 4.86 0.5144
WVFGRD96 66.0 90 70 20 4.87 0.5265
WVFGRD96 68.0 85 65 40 4.91 0.5465
WVFGRD96 70.0 85 70 40 4.92 0.5652
WVFGRD96 72.0 85 70 40 4.93 0.5847
WVFGRD96 74.0 85 70 40 4.93 0.6009
WVFGRD96 76.0 85 70 40 4.94 0.6155
WVFGRD96 78.0 85 70 45 4.95 0.6279
WVFGRD96 80.0 85 70 45 4.95 0.6393
WVFGRD96 82.0 85 70 45 4.95 0.6485
WVFGRD96 84.0 85 70 45 4.96 0.6555
WVFGRD96 86.0 85 75 45 4.96 0.6623
WVFGRD96 88.0 85 75 45 4.96 0.6679
WVFGRD96 90.0 85 75 45 4.96 0.6712
WVFGRD96 92.0 85 75 45 4.97 0.6736
WVFGRD96 94.0 85 75 45 4.97 0.6734
WVFGRD96 96.0 85 75 45 4.97 0.6726
WVFGRD96 98.0 85 75 45 4.97 0.6712
The best solution is
WVFGRD96 92.0 85 75 45 4.97 0.6736
The mechanism corresponding to the best fit is
|
|
|
The best fit as a function of depth is given in the following figure:
|
|
|
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 -50 o DIST/3.3 +30 rtr taper w 0.1 hp c 0.03 n 3 lp c 0.08 n 3
|
| 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. |
|
| 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