EMERGENCE OF DIRECT P-PHASE FROM SEISMIC AMBIENT NOISE IN DEHDASHT AREA

Publish Year: 1398
نوع سند: مقاله کنفرانسی
زبان: English
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شناسه ملی سند علمی:

SEE08_330

تاریخ نمایه سازی: 23 آبان 1399

Abstract:

The theoretical studies have revealed that cross correlation of seismic ambient noises can estimate the Green’s functions between a pair of stations (e.g. Snieder, 2004; Wapenaar, 2004). This idea encourages the researchers to do study using seismic ambient noise to determine the velocity structure. Several studies extracted the surface waves from seismic ambient noise and presented the corresponding surface wave tomography (e.g. Sabra et al., 2005; Bensen et al., 2007). In contrast, extraction of the body waves from the seismic ambient noise is still a critical issue, because the amplitude of the surface waves is dominant compared to the amplitude of body waves. However, some studies can retrieve the direct P wave (e.g. Roux, et al., 2005; Nakata et al., 2015, 2016) and reflected P wave (e.g. Draganov et al., 2009) from seismic ambient noises in local scale. In this study, we attempt to extract the direct P wave from seismic ambient noise data. We use the continues recorded ambient noises by an array network, including 120 broadband 3-component stations spaced about 2 km, installed in Dehdasht area, Iran. The data is recorded with a sample rate of 250 sps, however, it is decimated to 25 sps. To retrieve the P wave, we firstly separate the records to windows of 10 minutes (with no overlap) and calculate the Green’s function for all pair of stations via cross coherence formula of Nakata et al. (2015) for vertical (Z), radial (R) and transverse (T) components. Secondly, we linearly stack the corresponding cross coherency of the windows. To better extraction of the P wave, the suggested algorithm of Takagi et al. (2014) is used. This method requires full correlation tensor and is based on the polarization of the recorded noises, implying that the summation of ZR and RZ correlations eliminate the Rayleigh wave and retain the P wave. The complete expected phases from different types of correlations are listed in Table 1 (Takagi et al., 2014).

Authors

Ali RIAHI

Ph.D. Student in Geophysics, Institute of Geophysics, University of Tehran, Tehran, Iran

Zaher-Hossein SHOMALI

Associate Professor, Institute of Geophysics, University of Tehran, Tehran, Iran

Ahmad KAMAYESTANI

Ph.D. Candidate, The Islamic Azad University, Science and Research Branch, Tehran, Iran