Location

Location ANSS

Focal Mechanism

USGS/SLU Moment Tensor Solution ENS 2022/11/24 19:14:19:0 31.63 -103.98 7.0 4.5 Texas Stations used: 4O.MID02 GM.NMP25 GM.NMP41 GM.NMP44 GM.NMP45 GS.ALQ1 IM.TX31 IU.ANMO N4.ABTX N4.MSTX SC.121A SC.Y22A TX.ALPN TX.APMT TX.DKNS TX.MB01 TX.MB04 TX.MB05 TX.MB06 TX.MB09 TX.MB12 TX.ODSA TX.OZNA TX.PB05 TX.PB11 TX.PB21 TX.PB28 TX.PECS TX.POST TX.SAND TX.SGCY TX.SN08 TX.VHRN US.AMTX US.JCT US.MNTX 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 0.08 n 3 Best Fitting Double Couple Mo = 3.67e+22 dyne-cm Mw = 4.31 Z = 7 km Plane Strike Dip Rake NP1 120 55 -70 NP2 268 40 -116 Principal Axes: Axis Value Plunge Azimuth T 3.67e+22 8 196 N 0.00e+00 16 288 P -3.67e+22 72 81 Moment Tensor: (dyne-cm) Component Value Mxx 3.32e+22 Mxy 8.90e+21 Mxz -6.62e+21 Myy -8.03e+20 Myz -1.21e+22 Mzz -3.24e+22 ############## ###################### ############################ ############################## #############----------########### ########---------------------####### -#####---------------------------##### ---#---------------------------------### --##----------------------------------## --####------------------ --------------# -######----------------- P --------------- ########---------------- --------------- ##########-------------------------------- ###########----------------------------- ##############-------------------------- ################---------------------- ###################----------------- ################################## ############################## ############################ #### ############### T ########### Global CMT Convention Moment Tensor: R T P -3.24e+22 -6.62e+21 1.21e+22 -6.62e+21 3.32e+22 -8.90e+21 1.21e+22 -8.90e+21 -8.03e+20 Details of the solution is found at http://www.eas.slu.edu/eqc/eqc_mt/MECH.NA/20221124191419/index.html

Preferred Solution

      STK = 120
      DIP = 55
     RAKE = -70
       MW = 4.31
       HS = 7.0

The NDK file is 20221124191419.ndk The waveform inversion is preferred.

Moment Tensor Comparison

The following compares this source inversion to others

SLU

USGSMWR

USGS/SLU Moment Tensor Solution ENS 2022/11/24 19:14:19:0 31.63 -103.98 7.0 4.5 Texas Stations used: 4O.MID02 GM.NMP25 GM.NMP41 GM.NMP44 GM.NMP45 GS.ALQ1 IM.TX31 IU.ANMO N4.ABTX N4.MSTX SC.121A SC.Y22A TX.ALPN TX.APMT TX.DKNS TX.MB01 TX.MB04 TX.MB05 TX.MB06 TX.MB09 TX.MB12 TX.ODSA TX.OZNA TX.PB05 TX.PB11 TX.PB21 TX.PB28 TX.PECS TX.POST TX.SAND TX.SGCY TX.SN08 TX.VHRN US.AMTX US.JCT US.MNTX 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 0.08 n 3 Best Fitting Double Couple Mo = 3.67e+22 dyne-cm Mw = 4.31 Z = 7 km Plane Strike Dip Rake NP1 120 55 -70 NP2 268 40 -116 Principal Axes: Axis Value Plunge Azimuth T 3.67e+22 8 196 N 0.00e+00 16 288 P -3.67e+22 72 81 Moment Tensor: (dyne-cm) Component Value Mxx 3.32e+22 Mxy 8.90e+21 Mxz -6.62e+21 Myy -8.03e+20 Myz -1.21e+22 Mzz -3.24e+22 ############## ###################### ############################ ############################## #############----------########### ########---------------------####### -#####---------------------------##### ---#---------------------------------### --##----------------------------------## --####------------------ --------------# -######----------------- P --------------- ########---------------- --------------- ##########-------------------------------- ###########----------------------------- ##############-------------------------- ################---------------------- ###################----------------- ################################## ############################## ############################ #### ############### T ########### Global CMT Convention Moment Tensor: R T P -3.24e+22 -6.62e+21 1.21e+22 -6.62e+21 3.32e+22 -8.90e+21 1.21e+22 -8.90e+21 -8.03e+20 Details of the solution is found at http://www.eas.slu.edu/eqc/eqc_mt/MECH.NA/20221124191419/index.html

Moment Tensor Moment 3.458e+15 N-m Magnitude 4.29 Depth 7.0 km Percent DC 82% Half Duration - Catalog TX Data Source TX 1 Contributor TX 1 Nodal Planes Plane Strike Dip Rake NP1 321 69 -44 NP2 70 49 -152 Principal Axes Axis Value Plunge Azimuth T 3.607e+15 N-m 12 19 N -0.322e+15 N-m 42 120 P -3.286e+15 N-m 45 277

Magnitudes

ML Magnitude

(a) ML computed using the IASPEI formula for Horizontal components; (b) 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.

(a) ML computed using the IASPEI formula for Vertical components (research); (b) 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.

Context

Waveform Inversion using wvfgrd96

The focal mechanism was determined using broadband seismic waveforms. The location of the event and the and stations used for the waveform inversion are shown in the next figure.

Location of broadband stations used for waveform inversion

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 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 0.08 n 3 

           DEPTH  STK   DIP  RAKE   MW    FIT
WVFGRD96    1.0   150    75   -10   3.94 0.2174
WVFGRD96    2.0   145    55   -20   4.10 0.2583
WVFGRD96    3.0   135    90   -70   4.26 0.3256
WVFGRD96    4.0   320    90    65   4.26 0.3913
WVFGRD96    5.0   130    75   -60   4.26 0.4298
WVFGRD96    6.0   125    60   -65   4.29 0.4615
WVFGRD96    7.0   120    55   -70   4.31 0.4740
WVFGRD96    8.0   120    55   -70   4.37 0.4691
WVFGRD96    9.0   125    55   -65   4.37 0.4619
WVFGRD96   10.0   135    60   -50   4.36 0.4436
WVFGRD96   11.0   140    65   -40   4.36 0.4226
WVFGRD96   12.0   140    65   -40   4.36 0.4037
WVFGRD96   13.0   340    65    35   4.36 0.3905
WVFGRD96   14.0   340    65    35   4.36 0.3772
WVFGRD96   15.0   340    65    35   4.37 0.3651
WVFGRD96   16.0   340    65    30   4.37 0.3539
WVFGRD96   17.0   340    65    30   4.38 0.3428
WVFGRD96   18.0   340    65    30   4.38 0.3319
WVFGRD96   19.0   340    65    30   4.39 0.3218
WVFGRD96   20.0   340    65    25   4.39 0.3126
WVFGRD96   21.0   340    65    25   4.40 0.3041
WVFGRD96   22.0   340    65    25   4.41 0.2964
WVFGRD96   23.0   340    65    25   4.41 0.2894
WVFGRD96   24.0   340    65    25   4.42 0.2834
WVFGRD96   25.0   340    65    25   4.43 0.2781
WVFGRD96   26.0   340    65    20   4.43 0.2733
WVFGRD96   27.0   340    65    20   4.44 0.2692
WVFGRD96   28.0   340    60    20   4.45 0.2663
WVFGRD96   29.0   340    60    20   4.45 0.2636

The best solution is

WVFGRD96    7.0   120    55   -70   4.31 0.4740

The mechanism correspond to the best fit is

Figure 1. Waveform inversion focal mechanism

The best fit as a function of depth is given in the following figure:

Figure 2. Depth sensitivity for waveform mechanism

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 and because the velocity model used in the predictions may not be perfect. 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 0.08 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.

Focal mechanism sensitivity at the preferred depth. The red color indicates a very good fit to thewavefroms. 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:

• The origin time and epicentral distance are incorrect
• The velocity model used for the inversion is incorrect
• The velocity model used to define the P-arrival time is not the same as the velocity model used for the waveform inversion (assuming that the initial trace alignment is based on the P arrival time)

 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.

Discussion

Acknowledgements

Thanks also to the many seismic network operators whose dedication make this effort possible: University of Nevada Reno, University of Alaska, University of Washington, Oregon State University, University of Utah, Montana Bureau of Mines, UC Berkely, Caltech, UC San Diego, Saint Louis University, University of Memphis, Lamont Doherty Earth Observatory, the Oklahoma Geological Survey, TexNet, the Iris stations, the Transportable Array of EarthScope and other networks.

Velocity Model

The WUS.model used for the waveform synthetic seismograms and for the surface wave eigenfunctions and dispersion is as follows:

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    

Quality Control

Here we tabulate the reasons for not using certain digital data sets

The following stations did not have a valid response files: