Location

2012/03/05 15:15:06 44.540 9.377 10.5 4.1 Italy

Arrival Times (from USGS)

Arrival time list

Felt Map

USGS Felt map for this earthquake

USGS Felt reports page for

Focal Mechanism

 SLU Moment Tensor Solution
 ENS  2012/03/05 15:15:06:0  44.54    9.38  10.5 4.1 Italy
 
 Stations used:
   GU.BHB GU.MAIM GU.PCP GU.PZZ GU.RORO IV.ARCI IV.BDI IV.BOB 
   IV.CAFI IV.CRE IV.CRMI IV.DOI IV.FNVD IV.MSSA IV.PARC 
   IV.PLMA IV.QLNO IV.SALO MN.VLC 
 
 Filtering commands used:
   hp c 0.02 n 3
   lp c 0.10 n 3
 
 Best Fitting Double Couple
  Mo = 1.26e+22 dyne-cm
  Mw = 4.00 
  Z  = 7 km
  Plane   Strike  Dip  Rake
   NP1      112    56   -100
   NP2      310    35   -75
  Principal Axes:
   Axis    Value   Plunge  Azimuth
    T   1.26e+22     11     209
    N   0.00e+00      9     118
    P  -1.26e+22     76     350

 Moment Tensor: (dyne-cm)
    Component   Value
       Mxx     8.55e+21
       Mxy     5.30e+21
       Mxz    -4.90e+21
       Myy     2.88e+21
       Myz    -6.29e+20
       Mzz    -1.14e+22
                                                     
                                                     
                                                     
                                                     
                     ##############                  
                 ######################              
              #####------#################           
             ------------------############          
           ------------------------##########        
          ---------------------------#########       
         ------------------------------########      
        #-------------------------------########     
        ##----------------   -------------######     
       ####--------------- P --------------######    
       #####--------------   ---------------#####    
       #######------------------------------#####    
       #########-----------------------------####    
        ###########--------------------------###     
        ##############-----------------------###     
         #################-------------------#-      
          ########################------#####-       
           #################################-        
             ####   #######################          
              ### T ######################           
                    ###################              
                     ##############                  
                                                     
                                                     
                                                     
 Global CMT Convention Moment Tensor:
      R          T          P
 -1.14e+22  -4.90e+21   6.29e+20 
 -4.90e+21   8.55e+21  -5.30e+21 
  6.29e+20  -5.30e+21   2.88e+21 


Details of the solution is found at

http://www.eas.slu.edu/eqc/eqc_mt/MECH.IT/20120305151506/index.html
        

Preferred Solution

The preferred solution from an analysis of the surface-wave spectral amplitude radiation pattern, waveform inversion and first motion observations is

      STK = 310
      DIP = 35
     RAKE = -75
       MW = 4.00
       HS = 7.0

The waveform inversion is preferred.

Moment Tensor Comparison

The following compares this source inversion to others
SLU
INGVTDMT
 SLU Moment Tensor Solution
 ENS  2012/03/05 15:15:06:0  44.54    9.38  10.5 4.1 Italy
 
 Stations used:
   GU.BHB GU.MAIM GU.PCP GU.PZZ GU.RORO IV.ARCI IV.BDI IV.BOB 
   IV.CAFI IV.CRE IV.CRMI IV.DOI IV.FNVD IV.MSSA IV.PARC 
   IV.PLMA IV.QLNO IV.SALO MN.VLC 
 
 Filtering commands used:
   hp c 0.02 n 3
   lp c 0.10 n 3
 
 Best Fitting Double Couple
  Mo = 1.26e+22 dyne-cm
  Mw = 4.00 
  Z  = 7 km
  Plane   Strike  Dip  Rake
   NP1      112    56   -100
   NP2      310    35   -75
  Principal Axes:
   Axis    Value   Plunge  Azimuth
    T   1.26e+22     11     209
    N   0.00e+00      9     118
    P  -1.26e+22     76     350

 Moment Tensor: (dyne-cm)
    Component   Value
       Mxx     8.55e+21
       Mxy     5.30e+21
       Mxz    -4.90e+21
       Myy     2.88e+21
       Myz    -6.29e+20
       Mzz    -1.14e+22
                                                     
                                                     
                                                     
                                                     
                     ##############                  
                 ######################              
              #####------#################           
             ------------------############          
           ------------------------##########        
          ---------------------------#########       
         ------------------------------########      
        #-------------------------------########     
        ##----------------   -------------######     
       ####--------------- P --------------######    
       #####--------------   ---------------#####    
       #######------------------------------#####    
       #########-----------------------------####    
        ###########--------------------------###     
        ##############-----------------------###     
         #################-------------------#-      
          ########################------#####-       
           #################################-        
             ####   #######################          
              ### T ######################           
                    ###################              
                     ##############                  
                                                     
                                                     
                                                     
 Global CMT Convention Moment Tensor:
      R          T          P
 -1.14e+22  -4.90e+21   6.29e+20 
 -4.90e+21   8.55e+21  -5.30e+21 
  6.29e+20  -5.30e+21   2.88e+21 


Details of the solution is found at

http://www.eas.slu.edu/eqc/eqc_mt/MECH.IT/20120305151506/index.html
	

Waveform Inversion

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:

hp c 0.02 n 3
lp c 0.10 n 3
The results of this grid search from 0.5 to 19 km depth are as follow:

           DEPTH  STK   DIP  RAKE   MW    FIT
WVFGRD96    1.0   170    90   -50   3.70 0.2948
WVFGRD96    2.0   340    35   -20   3.80 0.3560
WVFGRD96    3.0   330    35   -40   3.84 0.4350
WVFGRD96    4.0   320    35   -65   3.90 0.5046
WVFGRD96    5.0   315    35   -70   3.99 0.5731
WVFGRD96    6.0   310    35   -75   4.01 0.6356
WVFGRD96    7.0   310    35   -75   4.00 0.6530
WVFGRD96    8.0   315    40   -70   3.97 0.6315
WVFGRD96    9.0   310    35   -75   3.97 0.6147
WVFGRD96   10.0   315    35   -70   3.97 0.5945
WVFGRD96   11.0   315    35   -70   3.97 0.5715
WVFGRD96   12.0   320    35   -65   3.97 0.5450
WVFGRD96   13.0   350    70    20   3.96 0.5266
WVFGRD96   14.0   350    70    20   3.97 0.5217
WVFGRD96   15.0   350    75    25   3.99 0.5071
WVFGRD96   16.0   355    70    25   4.00 0.5006
WVFGRD96   17.0   355    70    25   4.01 0.4940
WVFGRD96   18.0   355    70    25   4.02 0.4843
WVFGRD96   19.0   355    70    25   4.02 0.4774
WVFGRD96   20.0    -5    70    25   4.03 0.4673
WVFGRD96   21.0    -5    70    25   4.04 0.4582
WVFGRD96   22.0    -5    70    25   4.05 0.4483
WVFGRD96   23.0    -5    70    25   4.06 0.4387
WVFGRD96   24.0    -5    70    30   4.06 0.4305
WVFGRD96   25.0     0    65    30   4.07 0.4223
WVFGRD96   26.0     0    65    30   4.08 0.4127
WVFGRD96   27.0    35    40    30   4.11 0.4101
WVFGRD96   28.0    35    45    35   4.12 0.4138
WVFGRD96   29.0    35    45    35   4.13 0.4161

The best solution is

WVFGRD96    7.0   310    35   -75   4.00 0.6530

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

hp c 0.02 n 3
lp c 0.10 n 3
Figure 3. Waveform comparison for selected depth
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:

Assuming only a mislocation, the time shifts are fit to a functional form:

 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

Velocity Model

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    

Quality Control

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

The following stations did not have a valid response files:

DATE=Wed Mar 7 13:31:35 CST 2012

Last Changed 2012/03/05