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Body wave inversion of the 1970 and 1963 South American large deep-focus earthquakes

机译:1970年和1963年南美大深度地震的体波反演

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摘要

A comprehensive set of teleseismic waveforms from two South American deep-focus earthquakes of the predigital era, the 1970 Colombia (M_w = 8.1) and 1963 Peru-Bolivia (M_w = 7.7) events, are inverted for source mechanism, seismic moment, rupture history, and centroid depth. The P and SH wave inversion of the Colombia event confirms previous work, indicating that rupture occurred on a plane that dips steeply west. Rupture direction paralleled the trend of the Wadati-Benioff zone. We decompose the source into subevents, based on a source time function which shows two major moment release pulses separated by approx 20 s. The first subevent is located near the initiation point at a depth of approx 630 km. The main moment release was located approx 70 km to the southeast and approx 20 km shallower. Rupture subsequently propagated farther southeast. The source time function has an initial subevent accounting for approx 30% of the moment release of the entire event, whereas the long-period centroid moment tensor (CMT) analysis [Russakoff et al., 1997] has the initial subevent yielding approx 50%. The high-angle nodal plane rotated approx 15 deg clockwise during the rupture, explaining the large compensated linear vector dipole (CLVD) component inferred from CMT solutions. Individual subevents have large CLVD and compressive isotropic components. A full moment tensor inversion of the Colombia and 1994 Bolivia events suggests that the initial subevents might contain a large non-double-couple (NDC) component. For the 1963 Peru-Bolivia event, using P waves, rupture propagated NNW for a distance of approx 70 km, parallel to the high-angle nodal plane and the trend of the Wadati-Benioff zone. The focal mechanism changed dramatically after the second subevent, causing a very large NDC component. Both events, together with the 1994 Bolivia earthquake, have a precursor separated in space and time from the main rupture and show rupture velocities varying between 3 and 4 km/s between subevents, with <2.0 km/s on average for the entire event. Low seismic efficiencies and rupture velocities support a highly dissipative, temperature-dependent rupture mechanism for large deep-focus South American earthquakes, compared with events in cold subducting slabs.
机译:来自1970年哥伦比亚(M_w = 8.1)和1963年秘鲁-玻利维亚(M_w = 7.7)事件的两次南美深部数字地震的一组远震波形的综合震源波形被反转,用于震源机制,地震矩,破裂历史和质心深度。哥伦比亚事件的P波和SH波反演证实了先前的工作,表明破裂发生在向西倾斜的飞机上。破裂方向与Wadati-Benioff带的趋势平行。我们基于源时间函数将源分解为子事件,该函数显示两个主要的矩释放脉冲,相隔约20 s。第一个子事件位于起始点附近,深度约为630 km。主力矩释放位于东南约70公里处,较浅处约20公里处。破裂随后向东南传播。源时间函数的初始子事件约占整个事件的瞬间释放的30%,而长周期质心矩张量(CMT)分析[Russakoff等,1997]的初始子事件产生约50%的事件。 。在破裂过程中,高角度节点平面顺时针旋转了大约15度,解释了从CMT解决方案推断出的大补偿线性矢量偶极子(CLVD)分量。各个子事件具有较大的CLVD和压缩各向同性分量。哥伦比亚和1994年玻利维亚事件的一整张量张量反转表明,初始子事件可能包含较大的非双耦合(NDC)分量。对于1963年的秘鲁-玻利维亚事件,使用P波,破裂沿NNW传播了约70 km,与高角度节点平面和Wadati-Benioff带的走向平行。在第二个子事件之后,焦点机制发生了巨大变化,从而导致NDC分量很大。这两个事件以及1994年的玻利维亚地震,其前兆在时间和空间上都与主要破裂分开,子事件之间的破裂速度在3至4 km / s之间变化,整个事件的平均速度小于2.0 km / s。与冷俯冲板中的地震相比,低地震效率和破裂速度支持了高度耗散的,与温度有关的破裂机制,用于南美深部大型地震。

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