2016/09/01 11:35:57 42.5637 13.3038 12.1 3.7 L'Aquila
USGS Felt map for this earthquake
SLU Moment Tensor Solution ENS 2016/09/01 11:35:57:2 42.56 13.30 12.1 3.7 L'Aquila Stations used: IV.ARVD IV.ASQU IV.ASSB IV.ATTE IV.ATVO IV.CAFI IV.CERT IV.CESX IV.CING IV.CRE IV.FDMO IV.FIAM IV.FSSB IV.GUAR IV.GUMA IV.MA9 IV.MGAB IV.MODR IV.MTCE IV.MURB IV.NRCA IV.OFFI IV.PARC IV.POFI IV.PTQR IV.RMP IV.SACS IV.SNTG IV.TERO IV.TOLF Filtering commands used: cut o DIST/3.3 -20 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 = 1.29e+21 dyne-cm Mw = 3.34 Z = 6 km Plane Strike Dip Rake NP1 301 69 -112 NP2 170 30 -45 Principal Axes: Axis Value Plunge Azimuth T 1.29e+21 21 48 N 0.00e+00 21 309 P -1.29e+21 60 179 Moment Tensor: (dyne-cm) Component Value Mxx 1.80e+20 Mxy 5.63e+20 Mxz 8.56e+20 Myy 6.09e+20 Myz 3.12e+20 Mzz -7.89e+20 --############ ---################### ----######################## ----##################### ## -----###################### T #### #####--##################### ##### #####---------######################## ######-------------##################### #####------------------################# ######--------------------################ ######-----------------------############# ######-------------------------########### #######--------------------------######### ######----------------------------###### #######------------ -------------##### ######------------ P ---------------## ######----------- ---------------- #######--------------------------- ######------------------------ #######--------------------- ######---------------- ######-------- Global CMT Convention Moment Tensor: R T P -7.89e+20 8.56e+20 -3.12e+20 8.56e+20 1.80e+20 -5.63e+20 -3.12e+20 -5.63e+20 6.09e+20 Details of the solution is found at http://www.eas.slu.edu/eqc/eqc_mt/MECH.IT/20160901113557/index.html |
STK = 170 DIP = 30 RAKE = -45 MW = 3.34 HS = 6.0
The NDK file is 20160901113557.ndk The waveform inversion is preferred.
The following compares this source inversion to others
SLU Moment Tensor Solution ENS 2016/09/01 11:35:57:2 42.56 13.30 12.1 3.7 L'Aquila Stations used: IV.ARVD IV.ASQU IV.ASSB IV.ATTE IV.ATVO IV.CAFI IV.CERT IV.CESX IV.CING IV.CRE IV.FDMO IV.FIAM IV.FSSB IV.GUAR IV.GUMA IV.MA9 IV.MGAB IV.MODR IV.MTCE IV.MURB IV.NRCA IV.OFFI IV.PARC IV.POFI IV.PTQR IV.RMP IV.SACS IV.SNTG IV.TERO IV.TOLF Filtering commands used: cut o DIST/3.3 -20 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 = 1.29e+21 dyne-cm Mw = 3.34 Z = 6 km Plane Strike Dip Rake NP1 301 69 -112 NP2 170 30 -45 Principal Axes: Axis Value Plunge Azimuth T 1.29e+21 21 48 N 0.00e+00 21 309 P -1.29e+21 60 179 Moment Tensor: (dyne-cm) Component Value Mxx 1.80e+20 Mxy 5.63e+20 Mxz 8.56e+20 Myy 6.09e+20 Myz 3.12e+20 Mzz -7.89e+20 --############ ---################### ----######################## ----##################### ## -----###################### T #### #####--##################### ##### #####---------######################## ######-------------##################### #####------------------################# ######--------------------################ ######-----------------------############# ######-------------------------########### #######--------------------------######### ######----------------------------###### #######------------ -------------##### ######------------ P ---------------## ######----------- ---------------- #######--------------------------- ######------------------------ #######--------------------- ######---------------- ######-------- Global CMT Convention Moment Tensor: R T P -7.89e+20 8.56e+20 -3.12e+20 8.56e+20 1.80e+20 -5.63e+20 -3.12e+20 -5.63e+20 6.09e+20 Details of the solution is found at http://www.eas.slu.edu/eqc/eqc_mt/MECH.IT/20160901113557/index.html |
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.
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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 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 -20 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 from 0.5 to 19 km depth are as follow:
DEPTH STK DIP RAKE MW FIT WVFGRD96 1.0 325 40 -85 3.15 0.4362 WVFGRD96 2.0 180 25 -20 3.24 0.4808 WVFGRD96 3.0 180 30 -20 3.22 0.5795 WVFGRD96 4.0 180 35 -30 3.23 0.6357 WVFGRD96 5.0 175 30 -35 3.33 0.6833 WVFGRD96 6.0 170 30 -45 3.34 0.7037 WVFGRD96 7.0 175 35 -40 3.34 0.7027 WVFGRD96 8.0 180 40 -30 3.30 0.6814 WVFGRD96 9.0 185 45 -20 3.30 0.6660 WVFGRD96 10.0 185 45 -20 3.31 0.6490 WVFGRD96 11.0 185 45 -20 3.32 0.6287 WVFGRD96 12.0 185 45 -20 3.33 0.6061 WVFGRD96 13.0 190 50 -10 3.34 0.5825 WVFGRD96 14.0 190 45 -10 3.33 0.5587 WVFGRD96 15.0 190 45 -10 3.37 0.5372 WVFGRD96 16.0 190 45 -10 3.38 0.5121 WVFGRD96 17.0 190 45 -10 3.38 0.4880 WVFGRD96 18.0 185 45 -15 3.39 0.4651 WVFGRD96 19.0 185 45 -15 3.39 0.4446 WVFGRD96 20.0 110 75 50 3.40 0.4339 WVFGRD96 21.0 110 75 50 3.41 0.4269 WVFGRD96 22.0 110 75 50 3.42 0.4193 WVFGRD96 23.0 110 75 50 3.43 0.4104 WVFGRD96 24.0 110 75 50 3.44 0.4013 WVFGRD96 25.0 105 85 45 3.44 0.3915 WVFGRD96 26.0 105 85 45 3.45 0.3868 WVFGRD96 27.0 105 85 45 3.45 0.3827 WVFGRD96 28.0 105 85 45 3.46 0.3822 WVFGRD96 29.0 105 85 45 3.47 0.3803
The best solution is
WVFGRD96 6.0 170 30 -45 3.34 0.7037
The mechanism correspond 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 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 -20 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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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:
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 nnCIA used for the waveform synthetic seismograms and for the surface wave eigenfunctions and dispersion is as follows:
MODEL.01 C.It. A. Di Luzio et al Earth Plan Lettrs 280 (2009) 1-12 Fig 5. 7-8 MODEL/SURF3 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 1.5000 3.7497 2.1436 2.2753 0.500E-02 0.100E-01 0.00 0.00 1.00 1.00 3.0000 4.9399 2.8210 2.4858 0.500E-02 0.100E-01 0.00 0.00 1.00 1.00 3.0000 6.0129 3.4336 2.7058 0.500E-02 0.100E-01 0.00 0.00 1.00 1.00 7.0000 5.5516 3.1475 2.6093 0.167E-02 0.333E-02 0.00 0.00 1.00 1.00 15.0000 5.8805 3.3583 2.6770 0.167E-02 0.333E-02 0.00 0.00 1.00 1.00 6.0000 7.1059 4.0081 3.0002 0.167E-02 0.333E-02 0.00 0.00 1.00 1.00 8.0000 7.1000 3.9864 3.0120 0.167E-02 0.333E-02 0.00 0.00 1.00 1.00 0.0000 7.9000 4.4036 3.2760 0.167E-02 0.333E-02 0.00 0.00 1.00 1.00
Here we tabulate the reasons for not using certain digital data sets
The following stations did not have a valid response files:
DATE=Thu Sep 1 13:08:55 CDT 2016