The ANSS event ID is nc75458907 and the event page is at https://earthquake.usgs.gov/earthquakes/eventpage/nc75458907/executive.
2026/10/28 12:01:11 39.500 -122.952 10.6 4.0 California
USGS/SLU Moment Tensor Solution
ENS 2026/10/28 12:01:11.0 39.50 -122.95 10.6 4.0 California
Stations used:
BK.ADAM BK.ATP BK.AUSC BK.BARR BK.BEVN BK.BIGM BK.BJES
BK.BONV BK.BRIC BK.BUCI BK.DLIK BK.ETSL BK.GASB BK.GRPK
BK.GTSB BK.GUMB BK.HALS BK.HAYF BK.HOPS BK.HRCH BK.HUNT
BK.LCOS BK.MCCM BK.MLKN BK.MNRC BK.MORK BK.OAKV BK.ORRS
BK.PETY BK.PWOD BK.QRDG BK.RBOW BK.RVIT BK.SCOT BK.SHWD
BK.SNCR BK.SPAN BK.SPRL BK.USAL BK.VAK BK.WTWN NC.GCVB
NC.GDXB NC.GHGB NC.GRT NC.GSR NC.GSX NC.GTK NC.GWW NC.KCPC
NC.KNR NC.KRP NC.KTJ NC.KZE NC.NAPC NC.NBPB NC.NCO NC.NTO
NC.NTOM NC.NTR NC.NTYB
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 = 1.45e+22 dyne-cm
Mw = 4.04
Z = 14 km
Plane Strike Dip Rake
NP1 337 80 -170
NP2 245 80 -10
Principal Axes:
Axis Value Plunge Azimuth
T 1.45e+22 0 111
N 0.00e+00 76 20
P -1.45e+22 14 201
Moment Tensor: (dyne-cm)
Component Value
Mxx -1.00e+22
Mxy -9.34e+21
Mxz 3.18e+21
Myy 1.09e+22
Myz 1.24e+21
Mzz -8.58e+20
--------------
####------------------
########--------------------
###########-------------------
##############--------------------
################--------------------
##################-----------------###
####################---------###########
#####################---################
#####################--###################
#################------###################
##############----------##################
##########---------------#################
######-------------------#############
####---------------------############# T
#------------------------############
------------------------############
------------------------##########
----------------------########
------ -------------######
--- P -------------###
------------
Global CMT Convention Moment Tensor:
R T P
-8.58e+20 3.18e+21 -1.24e+21
3.18e+21 -1.00e+22 9.34e+21
-1.24e+21 9.34e+21 1.09e+22
Details of the solution is found at
http://www.eas.slu.edu/eqc/eqc_mt/MECH.NA/20261028120111/index.html
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STK = 245
DIP = 80
RAKE = -10
MW = 4.04
HS = 14.0
The NDK file is 20261028120111.ndk The waveform inversion is preferred.
The following compares this source inversion to those provided by others. The purpose is to look for major differences and also to note slight differences that might be inherent to the processing procedure. For completeness the USGS/SLU solution is repeated from above.
USGS/SLU Moment Tensor Solution
ENS 2026/10/28 12:01:11.0 39.50 -122.95 10.6 4.0 California
Stations used:
BK.ADAM BK.ATP BK.AUSC BK.BARR BK.BEVN BK.BIGM BK.BJES
BK.BONV BK.BRIC BK.BUCI BK.DLIK BK.ETSL BK.GASB BK.GRPK
BK.GTSB BK.GUMB BK.HALS BK.HAYF BK.HOPS BK.HRCH BK.HUNT
BK.LCOS BK.MCCM BK.MLKN BK.MNRC BK.MORK BK.OAKV BK.ORRS
BK.PETY BK.PWOD BK.QRDG BK.RBOW BK.RVIT BK.SCOT BK.SHWD
BK.SNCR BK.SPAN BK.SPRL BK.USAL BK.VAK BK.WTWN NC.GCVB
NC.GDXB NC.GHGB NC.GRT NC.GSR NC.GSX NC.GTK NC.GWW NC.KCPC
NC.KNR NC.KRP NC.KTJ NC.KZE NC.NAPC NC.NBPB NC.NCO NC.NTO
NC.NTOM NC.NTR NC.NTYB
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 = 1.45e+22 dyne-cm
Mw = 4.04
Z = 14 km
Plane Strike Dip Rake
NP1 337 80 -170
NP2 245 80 -10
Principal Axes:
Axis Value Plunge Azimuth
T 1.45e+22 0 111
N 0.00e+00 76 20
P -1.45e+22 14 201
Moment Tensor: (dyne-cm)
Component Value
Mxx -1.00e+22
Mxy -9.34e+21
Mxz 3.18e+21
Myy 1.09e+22
Myz 1.24e+21
Mzz -8.58e+20
--------------
####------------------
########--------------------
###########-------------------
##############--------------------
################--------------------
##################-----------------###
####################---------###########
#####################---################
#####################--###################
#################------###################
##############----------##################
##########---------------#################
######-------------------#############
####---------------------############# T
#------------------------############
------------------------############
------------------------##########
----------------------########
------ -------------######
--- P -------------###
------------
Global CMT Convention Moment Tensor:
R T P
-8.58e+20 3.18e+21 -1.24e+21
3.18e+21 -1.00e+22 9.34e+21
-1.24e+21 9.34e+21 1.09e+22
Details of the solution is found at
http://www.eas.slu.edu/eqc/eqc_mt/MECH.NA/20261028120111/index.html
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Moment Tensor (Mw) Moment 1.278e+15 N-m Magnitude 4.00 Mw Depth 14.0 km Percent DC 80% Half Duration - Catalog NC Data Source NC Contributor NC Nodal Planes Plane Strike Dip Rake NP1 246 85 -1 NP2 336 89 -175 Principal Axes Axis Value Plunge Azimuth T 1.340e+15 3 111 N -0.135e+15 85 347 P -1.205e+15 4 202 |
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.
Map showing station locations used for computing the ML's. No distinction is made whether the vertical (Z) or horizontal (H) components were used.
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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 1.0 245 90 0 3.41 0.2083
WVFGRD96 2.0 245 85 -5 3.58 0.3194
WVFGRD96 3.0 245 85 5 3.65 0.3665
WVFGRD96 4.0 245 85 20 3.71 0.4062
WVFGRD96 5.0 245 85 25 3.77 0.4444
WVFGRD96 6.0 245 90 -25 3.81 0.4862
WVFGRD96 7.0 245 90 -20 3.85 0.5246
WVFGRD96 8.0 65 90 25 3.90 0.5623
WVFGRD96 9.0 245 90 -25 3.93 0.5887
WVFGRD96 10.0 245 80 -20 3.96 0.6113
WVFGRD96 11.0 245 80 -15 3.98 0.6302
WVFGRD96 12.0 245 80 -15 4.01 0.6436
WVFGRD96 13.0 245 80 -15 4.02 0.6516
WVFGRD96 14.0 245 80 -10 4.04 0.6555
WVFGRD96 15.0 245 80 -10 4.06 0.6552
WVFGRD96 16.0 245 80 -10 4.07 0.6521
WVFGRD96 17.0 245 80 -10 4.08 0.6451
WVFGRD96 18.0 245 80 -10 4.09 0.6360
WVFGRD96 19.0 245 85 -10 4.10 0.6247
WVFGRD96 20.0 245 85 -10 4.11 0.6114
WVFGRD96 21.0 245 80 -10 4.12 0.5972
WVFGRD96 22.0 245 85 -10 4.12 0.5822
WVFGRD96 23.0 245 85 -10 4.12 0.5662
WVFGRD96 24.0 245 90 -15 4.13 0.5495
WVFGRD96 25.0 245 90 -15 4.13 0.5335
WVFGRD96 26.0 245 90 -15 4.13 0.5174
WVFGRD96 27.0 245 85 -15 4.13 0.5015
WVFGRD96 28.0 245 85 -15 4.13 0.4868
WVFGRD96 29.0 245 85 -15 4.13 0.4721
The best solution is
WVFGRD96 14.0 245 80 -10 4.04 0.6555
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