emporal variation of coda Q-1 associated with the occurrence of Dahaituoshan earthquake (ML= 5. 4) and its variation with the seismicity in Beijing area were studied by using 90 local earthquakes from the China Digita...emporal variation of coda Q-1 associated with the occurrence of Dahaituoshan earthquake (ML= 5. 4) and its variation with the seismicity in Beijing area were studied by using 90 local earthquakes from the China Digital Seismograph Network (CDSN). The results showed that there was a significant temporal change in coda Q-1 during the period from Jan. 1987 to Aug. 1991 and it was relative to the seismicity of this area. Coda Q-1 was determined for the lapse time window ranging from 10 to 60 s, frequency 1 to 16 Hz. By comparing the average values of Q-1 for different time periods, we found that in region near the mainshock area the coda Q-1 for earthquakes which occurred after the mainshock were higher than those earthquakes that occurred prior to the mainshock, while the coda Q-1 after the mainshock for the surrounding area were lower than before. We also found the temporal changes in η, the exponential in formula Q-1=Q0-1 (f/f0) -η, and Q0, the Q-factor at 1 Hz. Measurements of coda Q-1 from three components showed inconsistency in temporal variations for different frequencies.展开更多
文摘emporal variation of coda Q-1 associated with the occurrence of Dahaituoshan earthquake (ML= 5. 4) and its variation with the seismicity in Beijing area were studied by using 90 local earthquakes from the China Digital Seismograph Network (CDSN). The results showed that there was a significant temporal change in coda Q-1 during the period from Jan. 1987 to Aug. 1991 and it was relative to the seismicity of this area. Coda Q-1 was determined for the lapse time window ranging from 10 to 60 s, frequency 1 to 16 Hz. By comparing the average values of Q-1 for different time periods, we found that in region near the mainshock area the coda Q-1 for earthquakes which occurred after the mainshock were higher than those earthquakes that occurred prior to the mainshock, while the coda Q-1 after the mainshock for the surrounding area were lower than before. We also found the temporal changes in η, the exponential in formula Q-1=Q0-1 (f/f0) -η, and Q0, the Q-factor at 1 Hz. Measurements of coda Q-1 from three components showed inconsistency in temporal variations for different frequencies.