Location

2006/11/15 11:14:16 46.61 153.23 30

Moment Tensor Comparison

The following compares this source inversion to the USGS Rapid Moment Tensor Solution and to the Harvard CMT solutions, if they are available.
SLU
USGS
GLOBAL CMT
 SLU Moment Tensor Solution
 2006/11/15 11:14:16
 
 Best Fitting Double Couple
    Mo = 7.76e+27 dyne-cm
    Mw = 7.86 
    Z  = 110 km
     Plane   Strike  Dip  Rake
      NP1       30    70    80
      NP2      237    22   116
 Principal Axes:
   Axis    Value   Plunge  Azimuth
     T   7.76e+27     64     284
     N   0.00e+00      9      33
     P  -7.76e+27     24     128



 Moment Tensor: (dyne-cm)
    Component  Value
       Mxx    -2.33e+27
       Mxy     2.76e+27
       Mxz     2.53e+27
       Myy    -2.59e+27
       Myz    -5.30e+27
       Mzz     4.91e+27
                                                     
                                                     
                                                     
                                                     
                     --------------                  
                 ---------------------#              
              ---------###############-###           
             ------###################----#          
           ------#####################-------        
          -----#######################--------       
         ----########################----------      
        ----#########################-----------     
        ---#########################------------     
       ---##########   ############--------------    
       ---########## T ###########---------------    
       --###########   ##########----------------    
       --#######################-----------------    
        -######################-----------------     
        -#####################------------------     
         -###################----------   -----      
          #################------------ P ----       
           ##############--------------   ---        
             ###########-------------------          
              #######---------------------           
                 #---------------------              
                     --------------                  
                                                     
                                                     
                                                     

 Harvard Convention
 Moment Tensor:
      R          T          F
  4.91e+27   2.53e+27   5.30e+27 
  2.53e+27  -2.33e+27  -2.76e+27 
  5.30e+27  -2.76e+27  -2.59e+27 

	
6/11/15 11:14:16.76
 KURIL ISLANDS                   
 Epicenter:  46.683  153.224
 MW 7.9

 USGS MOMENT TENSOR SOLUTION
 Depth   7         No. of sta: 92
 Moment Tensor;   Scale 10**20 Nm
   Mrr= 3.58       Mtt=-4.14
   Mpp= 0.56       Mrt= 6.36
   Mrp= 4.16       Mtp=-1.87
  Principal axes:
   T  Val=  8.23  Plg=58  Azm=316
   N        0.94       8       60
   P       -9.17      31      155

 Best Double Couple:Mo=8.7*10**20
  NP1:Strike=270 Dip=16 Slip= 121
  NP2:        58     76        81
                                      
               -------                
          -----------------           
        -----###########-----         
      ---###################---       
    ---#######################---     
   --##########################-##    
   -#########   ##############---#    
  -########## T ############------#   
  ###########   ##########---------   
  #####################------------   
  ##################---------------   
  ###############------------------   
   ###########--------------------    
   #######------------   ---------    
    ------------------ P --------     
      ----------------   ------       
        ---------------------         
          -----------------           
               -------                

        
November 15, 2006, KURIL ISLANDS, MW=8.3

Meredith Nettles
Goran Ekstrom

CENTROID, MOMENT TENSOR SOLUTION
HARVARD EVENT-FILE NAME C111506A
DATA USED: GSN
L.P. BODY WAVES: 33S, 53C, T= 50
MANTLE WAVES:    79S,210C, T=200
CENTROID LOCATION:
ORIGIN TIME       11:15: 9.0 0.1
LAT 46.75N 0.01;LON 154.32E 0.01
DEP  13.4 0.6;HALF-DURATION 34.3
MOMENT TENSOR; SCALE 10**28 D-CM
  MRR= 1.67 0.01; MTT=-0.51 0.01
  MPP=-1.17 0.01; MRT= 1.57 0.11
  MRP= 2.47 0.15; MTP=-0.77 0.00
 PRINCIPAL AXES:
 1.(T) VAL=  3.37;PLG=60;AZM=302
 2.(N)       0.00;     0;     33
 3.(P)      -3.38;    30;    123
BEST DOUBLE COUPLE:M0=3.4*10**28
 NP1:STRIKE=214;DIP=15;SLIP=  92
 NP2:STRIKE= 33;DIP=75;SLIP=  90

            -----------           
        ----##############-       
      ---#################---     
    ---###################-----   
   ---###################-------  
  ---###################--------- 
  --#######   ##########--------- 
 --######## T #########-----------
 --########   ########------------
 --#################--------------
 --################---------------
  -###############--------   ---- 
  --#############--------- P ---- 
   -###########-----------   ---  
    -########------------------   
      -####------------------     
        #------------------       
            -----------           
        

Data set

The following broadband stations passed the QC and were used for the source inversion. AAK AAM AFI AGMN AMTX ANMO ANTO ARU BBSR BFO BINY BLA BMO BRAL BRVK BW06 CART CBKS CBN CHTO CMB CNNC COCO COLA COR CSS CTAO DAV DGMT DSB DUG DWPF ECSD EGAK EGMT ESK EYMN FUNA GNI GRFO GUMO HAWA HKT HLID HNR HRV HUMO HWUT ISP JCT JFWS KBS KEV KIEV KIV KONO KSU1 KURK KVTX KWP LAO LBNH LKWY LOHW LONY LTX MALT MBWA MCWV MNTX MOOW MORC MSO MVCO NCB NEW NWAO OBN OXF PAB PALK PFO PKME PMG POHA PSZ RAO RAR RGN RSSD SANT SAO SCIA SFJD SNOW SNZO SSPA STU SUMG SUW TATO TAU TLY TUC TZTN WLF WMOK WRAB WRAK WUAZ WVOR WVT

Deviatoric Moment Tensor Inversion

All observed and Greens function waveforms are corrected to instrument response to ground velocity in meters/sec for the passband of 0.004 - 5 Hz. The traces were then lowpass filtered at 0.25 Hz and interpolated to a sample rate of 1 second.

For the grid search, the observed traces and Green's functions are read in an cut using the following commands

Phase    Gsac Command              Comment
 P    cut A -30 A       CUTH = 95+0.3*DEPTH  
SH    cut T1 -60 T1     CUTH = 95+0.6*DEPTH
SV    cut T0 -60 T0     CUTH = 95+0.6*DEPTH

where the 95 is a maximum filter duration, DEPTH is in km, and the CUTH in sec
The cut windows attempt to include the P, pP, sP, pS, S and sS arrivals. However, oen must be very careful about the fact that PP may be included in some distance ranges.

The waveforms are then bandpass filtered by the application of the following high- and low-pass stages (an optional microseism filter):

hp c 0.0050 2
lp c 0.0100 2
int
br c 0.12 0.2 n 4 p 2
The traces were next integrated to ground displacment in meters. Finally the observed data are interpolated to ahve the same sampling at the Green's functions.
NOTE: this was done for speed. The proper sequence is to read traces, filter and then cut - gsac will be modified to introduce a command CUTWR to define the cut upon a write.

The source inversion is a multipass operation since a lower frequency filter band is used for larger earthquakes and since a search is made over depth. Up to three passed of the outer loop are made, after which the moment magnitude is determined and filter settings readjusted. The inner loop over depth samples all depths from 0 to 800 km with 5 km increments in depth to 50 km, followed by 10 km depth sampling for the remaining range.

The following filter ranges are used according to the moment magnitude Mw:

   FILTER_BAND   FH(s)  FL(s)
       1           60     12      Mw < 6.4
       2          100     20      6.4 < Mw <= 6.9
       3          120     40      Mw > 6.9

The map displays the distribution of stations used for this source inversion.


Location of the earthquake (yellow star) and great circle path from the epicenter to each station (red) [created using GMT (Wessel, P., and W. H. F. Smith, New version of Generic Mapping Tools released, EOS Trans. AGU, 76 329, 1995.)]

For this data set the favored solution is

WVFMTD96  200.0   30.   63.   86.   7.92     0.433 0.165E-03     0.458     0.659 0.694E-04  24.9

The following figures show the sensitivity of the goodness of fit parameter so source depth, the waveform comparison as a function of epicentral distance in degrees and the source to station azimuth

Depth Sensitivity

Goodness of fit as a function of source depth. The measure is 1 - SUM (o -p)2 / SUM o2. A value of 1.0 is the best fit. The best double couple mechanism for the solution depth is plotted above goodness of fit value to indicate how the mefhanism may change with depth.

Detailed Waveform Comparison

P-wave Z component
Comparison of the observed traces (red) and solution predicted traces (blue) ordered in terms of increasing epicentral distance. Each pair of traces is annotated with the station name, epicentral distance in degrees, source to station azimuth in degrees. Each pair of traces is plotted with the same scale and the peak amplitudes are indicated at the lect of each trace. Finally the time shift between the P-wave first arrival picked and the the theoretical P-wave first arrival in the predicted trace is indicated, with a positive sign indicating that the predicted trace has been shifted to the right by the given number of seconds. as a function of source to station azimuth in degrees (D). The purpose of this display is to highlight the azimuthal dependence on the first motion. The traces are annotated with the station name at the top.
SH-wave T component
Comparison of the observed traces (red) and solution predicted traces (blue) ordered in terms of increasing epicentral distance. Each pair of traces is annotated with the station name, epicentral distance in degrees, source to station azimuth in degrees. Each pair of traces is plotted with the same scale and the peak amplitudes are indicated at the lect of each trace. Finally the time shift between the P-wave first arrival picked and the the theoretical P-wave first arrival in the predicted trace is indicated, with a positive sign indicating that the predicted trace has been shifted to the right by the given number of seconds. as a function of source to station azimuth in degrees (D). The purpose of this display is to highlight the azimuthal dependence on the first motion. The traces are annotated with the station name at the top.
SV-wave R component
Comparison of the observed traces (red) and solution predicted traces (blue) ordered in terms of increasing epicentral distance. Each pair of traces is annotated with the station name, epicentral distance in degrees, source to station azimuth in degrees. Each pair of traces is plotted with the same scale and the peak amplitudes are indicated at the lect of each trace. Finally the time shift between the P-wave first arrival picked and the the theoretical P-wave first arrival in the predicted trace is indicated, with a positive sign indicating that the predicted trace has been shifted to the right by the given number of seconds. as a function of source to station azimuth in degrees (D). The purpose of this display is to highlight the azimuthal dependence on the first motion. The traces are annotated with the station name at the top.

Inversion Details

Output of wvfmtd96 for the best depth..

Grid Search

All observed and Greens function waveforms are corrected to instrument response to ground velocity in meters/sec for the passband of 0.004 - 5 Hz. The traces were then lowpass filtered at 0.25 Hz and interpolated to a sample rate of 1 second.

For the grid search, the observed traces and Green's functions are read in an cut using the following commands

Phase    Gsac Command              Comment
 P    cut A -30 A       CUTH = 95+0.3*DEPTH  
SH    cut T1 -60 T1     CUTH = 95+0.6*DEPTH
SV    cut T0 -60 T0     CUTH = 95+0.6*DEPTH

where the 95 is a maximum filter duration, DEPTH is in km, and the CUTH in sec
The cut windows attempt to include the P, pP, sP, pS, S and sS arrivals. However, oen must be very careful about the fact that PP may be included in some distance ranges.

The waveforms are then bandpass filtered by the application of the following high- and low-pass stages (an optional microseism filter):

hp c 0.0050 2
lp c 0.0100 2
int
br c 0.12 0.2 n 4 p 2
The traces were next integrated to ground displacment in meters. Finally the observed data are interpolated to ahve the same sampling at the Green's functions.
NOTE: this was done for speed. The proper sequence is to read traces, filter and then cut - gsac will be modified to introduce a command CUTWR to define the cut upon a write.

The source inversion is a multipass operation since a lower frequency filter band is used for larger earthquakes and since a search is made over depth. Up to three passed of the outer loop are made, after which the moment magnitude is determined and filter settings readjusted. The inner loop over depth samples all depths from 0 to 800 km with 5 km increments in depth to 50 km, followed by 10 km depth sampling for the remaining range.

The following filter ranges are used according to the moment magnitude Mw:

   FILTER_BAND   FH(s)  FL(s)
       1           60     12      Mw < 6.4
       2          100     20      6.4 < Mw <= 6.9
       3          120     40      Mw > 6.9

The map displays the distribution of stations used for this source inversion.


Location of the earthquake (yellow star) and great circle path from the epicenter to each station (red) [created using GMT (Wessel, P., and W. H. F. Smith, New version of Generic Mapping Tools released, EOS Trans. AGU, 76 329, 1995.)]

For this data set the favored solution is

WVFGRD96  110.0    30    70    80   7.86 0.5539

The following figures show the sensitivity of the goodness of fit parameter so source depth, the waveform comparison as a function of epicentral distance in degrees and the source to station azimuth

Depth Sensitivity

Goodness of fit as a function of source depth. The measure is 1 - SUM (o -p)2 / SUM o2. A value of 1.0 is the best fit. The best double couple mechanism for the solution depth is plotted above goodness of fit value to indicate how the mefhanism may change with depth.

Detailed Waveform Comparison

P-wave Z component
Comparison of the observed traces (red) and solution predicted traces (blue) ordered in terms of increasing epicentral distance. Each pair of traces is annotated with the station name, epicentral distance in degrees, source to station azimuth in degrees. Each pair of traces is plotted with the same scale and the peak amplitudes are indicated at the lect of each trace. Finally the time shift between the P-wave first arrival picked and the the theoretical P-wave first arrival in the predicted trace is indicated, with a positive sign indicating that the predicted trace has been shifted to the right by the given number of seconds. as a function of source to station azimuth in degrees (D). The purpose of this display is to highlight the azimuthal dependence on the first motion. The traces are annotated with the station name at the top.
SH-wave T component
Comparison of the observed traces (red) and solution predicted traces (blue) ordered in terms of increasing epicentral distance. Each pair of traces is annotated with the station name, epicentral distance in degrees, source to station azimuth in degrees. Each pair of traces is plotted with the same scale and the peak amplitudes are indicated at the lect of each trace. Finally the time shift between the P-wave first arrival picked and the the theoretical P-wave first arrival in the predicted trace is indicated, with a positive sign indicating that the predicted trace has been shifted to the right by the given number of seconds. as a function of source to station azimuth in degrees (D). The purpose of this display is to highlight the azimuthal dependence on the first motion. The traces are annotated with the station name at the top.
SV-wave R component
Comparison of the observed traces (red) and solution predicted traces (blue) ordered in terms of increasing epicentral distance. Each pair of traces is annotated with the station name, epicentral distance in degrees, source to station azimuth in degrees. Each pair of traces is plotted with the same scale and the peak amplitudes are indicated at the lect of each trace. Finally the time shift between the P-wave first arrival picked and the the theoretical P-wave first arrival in the predicted trace is indicated, with a positive sign indicating that the predicted trace has been shifted to the right by the given number of seconds. as a function of source to station azimuth in degrees (D). The purpose of this display is to highlight the azimuthal dependence on the first motion. The traces are annotated with the station name at the top.

Inversion Details

Output of wvfgrd96 for the best depth..

Last Changed Thu Apr 12 20:50:13 UTC 2007