The ANSS event ID is us7000477q and the event page is at https://earthquake.usgs.gov/earthquakes/eventpage/us7000477q/executive.
2019/06/29 07:58:59 36.391 -113.824 6.4 3.8 Arizona
USGS/SLU Moment Tensor Solution ENS 2019/06/29 07:58:59:0 36.39 -113.82 6.4 3.8 Arizona Stations used: AE.113A AE.BABIT AE.BARN AE.PRCT AE.TONTO AE.U15A AE.W13A AE.W18A AE.X16A AE.X18A AE.Y14A CI.BLY CI.CCA CI.GLA CI.GRA CI.GSC CI.ISA CI.LDF CI.RAG II.PFO LB.MVU LB.TPH NN.DSP NN.GWY NN.MZPB NN.PIO NN.PRN NN.Q09A NN.QSM NN.R11B NN.S11A NN.SHP NN.SPR3 NN.V12A NN.WLDB SN.HEL US.DUG US.TPNV US.WUAZ UU.CVRU UU.HMU UU.KNB UU.LCMT UU.MPU UU.PSUT UU.SRU UU.TMU UU.VRUT 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 = 6.53e+21 dyne-cm Mw = 3.81 Z = 16 km Plane Strike Dip Rake NP1 187 50 -113 NP2 40 45 -65 Principal Axes: Axis Value Plunge Azimuth T 6.53e+21 3 293 N 0.00e+00 17 202 P -6.53e+21 72 31 Moment Tensor: (dyne-cm) Component Value Mxx 5.24e+20 Mxy -2.58e+21 Mxz -1.50e+21 Myy 5.40e+21 Myz -1.25e+21 Mzz -5.92e+21 #######------- #########------------- ##########-----------------# ##########-------------------# ##########----------------------## ##########----------------------### T #########-----------------------#### ########---------- -----------##### ###########---------- P ----------###### ###########----------- ----------####### ###########-----------------------######## ###########-----------------------######## ###########----------------------######### ##########---------------------######### ##########-------------------########### #########------------------########### #########---------------############ #########-----------############## #######--------############### #######---################## ------################ ---########### Global CMT Convention Moment Tensor: R T P -5.92e+21 -1.50e+21 1.25e+21 -1.50e+21 5.24e+20 2.58e+21 1.25e+21 2.58e+21 5.40e+21 Details of the solution is found at http://www.eas.slu.edu/eqc/eqc_mt/MECH.NA/20190629075859/index.html |
STK = 40 DIP = 45 RAKE = -65 MW = 3.81 HS = 16.0
The NDK file is 20190629075859.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: mLg computed using the IASPEI formula. Center: mLg residuals versus epicentral distance ; the values used for the trimmed mean magnitude estimate are indicated.
Right: residuals as a function of distance and azimuth.
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 0.08 n 3The results of this grid search are as follow:
DEPTH STK DIP RAKE MW FIT WVFGRD96 1.0 20 45 -90 3.43 0.3107 WVFGRD96 2.0 20 45 -90 3.54 0.3644 WVFGRD96 3.0 70 80 15 3.44 0.2657 WVFGRD96 4.0 20 85 -75 3.60 0.3189 WVFGRD96 5.0 20 85 -75 3.60 0.3788 WVFGRD96 6.0 20 85 -75 3.61 0.4231 WVFGRD96 7.0 20 85 -75 3.61 0.4545 WVFGRD96 8.0 20 85 -75 3.69 0.4759 WVFGRD96 9.0 10 20 75 3.72 0.5036 WVFGRD96 10.0 10 25 75 3.74 0.5334 WVFGRD96 11.0 10 30 75 3.75 0.5570 WVFGRD96 12.0 35 55 -75 3.77 0.5707 WVFGRD96 13.0 35 40 -70 3.78 0.5935 WVFGRD96 14.0 35 45 -70 3.79 0.6088 WVFGRD96 15.0 40 45 -65 3.80 0.6173 WVFGRD96 16.0 40 45 -65 3.81 0.6197 WVFGRD96 17.0 40 45 -65 3.81 0.6173 WVFGRD96 18.0 40 45 -65 3.82 0.6108 WVFGRD96 19.0 45 45 -55 3.82 0.6012 WVFGRD96 20.0 45 45 -55 3.83 0.5900 WVFGRD96 21.0 45 45 -55 3.84 0.5775 WVFGRD96 22.0 45 45 -55 3.85 0.5628 WVFGRD96 23.0 45 45 -55 3.85 0.5468 WVFGRD96 24.0 45 40 -55 3.86 0.5300 WVFGRD96 25.0 45 40 -55 3.86 0.5128 WVFGRD96 26.0 45 40 -50 3.86 0.4953 WVFGRD96 27.0 45 40 -50 3.87 0.4772 WVFGRD96 28.0 45 40 -50 3.87 0.4583 WVFGRD96 29.0 45 40 -50 3.88 0.4385
The best solution is
WVFGRD96 16.0 40 45 -65 3.81 0.6197
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 0.08 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