2015/01/23 09:56:15 44.136 11.149 10.0 3.4 Italy
USGS Felt map for this earthquake
SLU Moment Tensor Solution ENS 2015/01/23 09:56:15:0 44.14 11.15 10.0 3.4 Italy Stations used: GU.MAIM IV.ARVD IV.ASQU IV.ATFO IV.ATPC IV.BDI IV.BOB IV.CAFI IV.CASP IV.CESI IV.CING IV.CRE IV.CSNT IV.FDMO IV.GROG IV.MGAB IV.MSSA IV.MTRZ IV.MURB IV.OSSC IV.PARC IV.PIEI IV.PLMA IV.SACS IV.ZCCA MN.VLC Filtering commands used: cut o DIST/3.3 -30 o DIST/3.3 +70 rtr taper w 0.1 hp c 0.02 n 3 lp c 0.10 n 3 Best Fitting Double Couple Mo = 5.31e+21 dyne-cm Mw = 3.75 Z = 6 km Plane Strike Dip Rake NP1 120 55 -85 NP2 291 35 -97 Principal Axes: Axis Value Plunge Azimuth T 5.31e+21 10 206 N 0.00e+00 4 297 P -5.31e+21 79 49 Moment Tensor: (dyne-cm) Component Value Mxx 4.06e+21 Mxy 1.96e+21 Mxz -1.43e+21 Myy 9.14e+20 Myz -1.13e+21 Mzz -4.97e+21 ############## ###################### ############################ #######--------############### ###--------------------########### #---------------------------######## #------------------------------####### ###-------------------------------###### ####------------------ ----------##### ######----------------- P ------------#### #######---------------- -------------### ########-------------------------------### ##########------------------------------## ###########----------------------------# ##############-------------------------# ################---------------------- ###################----------------- ################################## ############################## #### ##################### # T ################## ############## Global CMT Convention Moment Tensor: R T P -4.97e+21 -1.43e+21 1.13e+21 -1.43e+21 4.06e+21 -1.96e+21 1.13e+21 -1.96e+21 9.14e+20 Details of the solution is found at http://www.eas.slu.edu/eqc/eqc_mt/MECH.IT/20150123095615/index.html |
STK = 120 DIP = 55 RAKE = -85 MW = 3.75 HS = 6.0
The NDK file is 20150123095615.ndk The waveform inversion is preferred.
The following compares this source inversion to others
SLU Moment Tensor Solution ENS 2015/01/23 09:56:15:0 44.14 11.15 10.0 3.4 Italy Stations used: GU.MAIM IV.ARVD IV.ASQU IV.ATFO IV.ATPC IV.BDI IV.BOB IV.CAFI IV.CASP IV.CESI IV.CING IV.CRE IV.CSNT IV.FDMO IV.GROG IV.MGAB IV.MSSA IV.MTRZ IV.MURB IV.OSSC IV.PARC IV.PIEI IV.PLMA IV.SACS IV.ZCCA MN.VLC Filtering commands used: cut o DIST/3.3 -30 o DIST/3.3 +70 rtr taper w 0.1 hp c 0.02 n 3 lp c 0.10 n 3 Best Fitting Double Couple Mo = 5.31e+21 dyne-cm Mw = 3.75 Z = 6 km Plane Strike Dip Rake NP1 120 55 -85 NP2 291 35 -97 Principal Axes: Axis Value Plunge Azimuth T 5.31e+21 10 206 N 0.00e+00 4 297 P -5.31e+21 79 49 Moment Tensor: (dyne-cm) Component Value Mxx 4.06e+21 Mxy 1.96e+21 Mxz -1.43e+21 Myy 9.14e+20 Myz -1.13e+21 Mzz -4.97e+21 ############## ###################### ############################ #######--------############### ###--------------------########### #---------------------------######## #------------------------------####### ###-------------------------------###### ####------------------ ----------##### ######----------------- P ------------#### #######---------------- -------------### ########-------------------------------### ##########------------------------------## ###########----------------------------# ##############-------------------------# ################---------------------- ###################----------------- ################################## ############################## #### ##################### # T ################## ############## Global CMT Convention Moment Tensor: R T P -4.97e+21 -1.43e+21 1.13e+21 -1.43e+21 4.06e+21 -1.96e+21 1.13e+21 -1.96e+21 9.14e+20 Details of the solution is found at http://www.eas.slu.edu/eqc/eqc_mt/MECH.IT/20150123095615/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 -30 o DIST/3.3 +70 rtr taper w 0.1 hp c 0.02 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 1.0 120 45 -80 3.48 0.2437 WVFGRD96 2.0 150 75 -55 3.53 0.2681 WVFGRD96 3.0 140 70 -65 3.58 0.3114 WVFGRD96 4.0 120 60 -85 3.64 0.3654 WVFGRD96 5.0 120 60 -85 3.74 0.4344 WVFGRD96 6.0 120 55 -85 3.75 0.4695 WVFGRD96 7.0 120 55 -85 3.74 0.4683 WVFGRD96 8.0 120 55 -85 3.71 0.4496 WVFGRD96 9.0 290 35 -100 3.71 0.4458 WVFGRD96 10.0 125 60 -80 3.71 0.4401 WVFGRD96 11.0 125 60 -80 3.72 0.4306 WVFGRD96 12.0 295 25 -95 3.73 0.4202 WVFGRD96 13.0 345 75 25 3.71 0.4147 WVFGRD96 14.0 160 90 -30 3.72 0.4088 WVFGRD96 15.0 155 80 -40 3.75 0.4057 WVFGRD96 16.0 155 85 -40 3.76 0.3986 WVFGRD96 17.0 155 85 -40 3.76 0.3918 WVFGRD96 18.0 340 85 30 3.77 0.3822 WVFGRD96 19.0 340 85 30 3.77 0.3751 WVFGRD96 20.0 340 80 30 3.78 0.3665 WVFGRD96 21.0 340 80 30 3.79 0.3599 WVFGRD96 22.0 340 75 30 3.79 0.3542 WVFGRD96 23.0 340 75 30 3.80 0.3495 WVFGRD96 24.0 340 75 30 3.81 0.3458 WVFGRD96 25.0 345 70 30 3.82 0.3420 WVFGRD96 26.0 345 70 30 3.83 0.3380 WVFGRD96 27.0 345 70 30 3.84 0.3346 WVFGRD96 28.0 320 70 -50 3.88 0.3328 WVFGRD96 29.0 345 70 30 3.87 0.3332
The best solution is
WVFGRD96 6.0 120 55 -85 3.75 0.4695
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 -30 o DIST/3.3 +70 rtr taper w 0.1 hp c 0.02 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=Sat Jan 24 16:14:18 CST 2015