2009/04/06 23:49:34 42.349 13.378 8.3 3.00 Italy
USGS Felt map for this earthquake
USGS/SLU Moment Tensor Solution ENS 2009/04/06 23:49:34:0 42.35 13.38 8.3 3.0 Italy Stations used: IV.ASSB IV.CAFR IV.FAGN IV.FDMO IV.FIAM IV.INTR IV.MIDA IV.MNS IV.OFFI IV.TERO Filtering commands used: hp c 0.02 n 3 lp c 0.10 n 3 Best Fitting Double Couple Mo = 7.94e+20 dyne-cm Mw = 3.20 Z = 5 km Plane Strike Dip Rake NP1 155 50 -60 NP2 293 48 -121 Principal Axes: Axis Value Plunge Azimuth T 7.94e+20 1 224 N 0.00e+00 23 315 P -7.94e+20 67 132 Moment Tensor: (dyne-cm) Component Value Mxx 3.54e+20 Mxy 4.55e+20 Mxz 1.81e+20 Myy 3.23e+20 Myz -2.16e+20 Mzz -6.77e+20 ############## -##################### ----######################## ----########################## -----############################# --####---------------############### #######-------------------############ ########----------------------########## ########------------------------######## ##########-------------------------####### ##########--------------------------###### ###########---------------------------#### ###########------------- ------------### ###########------------ P ------------## ############----------- -------------# ############-------------------------- #############----------------------- #############--------------------- ##########----------------- T ############-------------- ###############------- ############## Global CMT Convention Moment Tensor: R T P -6.77e+20 1.81e+20 2.16e+20 1.81e+20 3.54e+20 -4.55e+20 2.16e+20 -4.55e+20 3.23e+20 Details of the solution is found at http://www.eas.slu.edu/eqc/eqc_mt/MECH.IT/20090406234934/index.html |
STK = 155 DIP = 50 RAKE = -60 MW = 3.20 HS = 5.0
The waveform inversion is preferred.
The following compares this source inversion to others
USGS/SLU Moment Tensor Solution ENS 2009/04/06 23:49:34:0 42.35 13.38 8.3 3.0 Italy Stations used: IV.ASSB IV.CAFR IV.FAGN IV.FDMO IV.FIAM IV.INTR IV.MIDA IV.MNS IV.OFFI IV.TERO Filtering commands used: hp c 0.02 n 3 lp c 0.10 n 3 Best Fitting Double Couple Mo = 7.94e+20 dyne-cm Mw = 3.20 Z = 5 km Plane Strike Dip Rake NP1 155 50 -60 NP2 293 48 -121 Principal Axes: Axis Value Plunge Azimuth T 7.94e+20 1 224 N 0.00e+00 23 315 P -7.94e+20 67 132 Moment Tensor: (dyne-cm) Component Value Mxx 3.54e+20 Mxy 4.55e+20 Mxz 1.81e+20 Myy 3.23e+20 Myz -2.16e+20 Mzz -6.77e+20 ############## -##################### ----######################## ----########################## -----############################# --####---------------############### #######-------------------############ ########----------------------########## ########------------------------######## ##########-------------------------####### ##########--------------------------###### ###########---------------------------#### ###########------------- ------------### ###########------------ P ------------## ############----------- -------------# ############-------------------------- #############----------------------- #############--------------------- ##########----------------- T ############-------------- ###############------- ############## Global CMT Convention Moment Tensor: R T P -6.77e+20 1.81e+20 2.16e+20 1.81e+20 3.54e+20 -4.55e+20 2.16e+20 -4.55e+20 3.23e+20 Details of the solution is found at http://www.eas.slu.edu/eqc/eqc_mt/MECH.IT/20090406234934/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.
![]() |
|
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:
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 0.5 150 55 -70 2.96 0.3219 WVFGRD96 1.0 165 60 -55 2.99 0.3441 WVFGRD96 2.0 165 60 -55 3.07 0.4081 WVFGRD96 3.0 165 55 -50 3.09 0.4471 WVFGRD96 4.0 165 55 -50 3.11 0.4516 WVFGRD96 5.0 155 50 -60 3.20 0.4707 WVFGRD96 6.0 165 55 -50 3.17 0.4351 WVFGRD96 7.0 175 65 -35 3.15 0.4062 WVFGRD96 8.0 180 75 -25 3.14 0.3873 WVFGRD96 9.0 180 75 -25 3.15 0.3826 WVFGRD96 10.0 180 75 -25 3.16 0.3753 WVFGRD96 11.0 180 75 -25 3.17 0.3676 WVFGRD96 12.0 180 70 -25 3.18 0.3601 WVFGRD96 13.0 135 80 35 3.25 0.3648 WVFGRD96 14.0 135 80 40 3.25 0.3696 WVFGRD96 15.0 135 80 40 3.29 0.3731 WVFGRD96 16.0 135 80 40 3.30 0.3770 WVFGRD96 17.0 310 90 -40 3.32 0.3721 WVFGRD96 18.0 135 80 40 3.32 0.3779 WVFGRD96 19.0 310 90 -40 3.34 0.3746 WVFGRD96 20.0 130 90 40 3.35 0.3736 WVFGRD96 21.0 130 90 40 3.36 0.3699 WVFGRD96 22.0 310 90 -40 3.37 0.3668 WVFGRD96 23.0 130 85 40 3.37 0.3663 WVFGRD96 24.0 310 90 -35 3.39 0.3662 WVFGRD96 25.0 310 90 -35 3.40 0.3683 WVFGRD96 26.0 310 90 -35 3.41 0.3699 WVFGRD96 27.0 310 90 -35 3.42 0.3688 WVFGRD96 28.0 135 80 35 3.41 0.3710 WVFGRD96 29.0 135 85 30 3.44 0.3692
The best solution is
WVFGRD96 5.0 155 50 -60 3.20 0.4707
The mechanism correspond to the best fit is
![]() |
|
The best fit as a function of depth is given in the following figure:
![]() |
|
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. The number in black at the rightr of each predicted traces 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 bandpass filter used in the processing and for the display was
hp c 0.02 n 3 lp c 0.10 n 3
![]() |
|
![]() |
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. |
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=Fri May 1 15:00:49 CDT 2009