4.6 Article

Attenuation of high-frequency seismic waves in northeast India

Journal

GEOPHYSICAL JOURNAL INTERNATIONAL
Volume 181, Issue 1, Pages 453-467

Publisher

OXFORD UNIV PRESS
DOI: 10.1111/j.1365-246X.2010.04502.x

Keywords

Body waves; Coda waves; Seismic attenuation; Wave propagation

Funding

  1. Council of Scientific and Industrial Research
  2. Department of Science and Technology, New Delhi, Govt. of India

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We studied attenuation of S and coda waves, their frequency and lapse time dependencies in northeast India in the frequency range of 1-24 Hz. We adopted theories of both single and multiple scattering to bandpass-filtered seismograms to fit coda envelopes to estimate Q for coda waves (Q(C)) and Q for S-waves (Q(S)) at five central frequencies of 1.5, 3, 6, 12 and 24 Hz. The selected data set consists of 182 seismograms recorded at ten seismic stations within epicentral distance of 22-300 km in the local magnitude range of 2.5-5.2. We found that with the increase in lapse time window from 40 to 60 s, Q(0) (Q(C) at 1 Hz) increases from 213 to 278, while the frequency dependent coefficient n decreases from 0.89 to 0.79. Both Q(C) and QS increase with frequency. The average value of QS obtained by using coda normalization method for NE India has the power law form of (96.8 +/- 21.5)(f(1.03+/-0.04)) in 1-24 Hz. We adopted energy flux model (EFM) and diffusion model for the multiple scattered wave energy in three-dimensions. The results show that the contribution of multiple scattering dominates for longer lapse time close to or larger than mean free time of about 60 s. The estimates of Q(C) are overestimated at longer lapse time by neglecting the effects of multiple scattering. Some discrepancies have been observed between the theoretical predictions and the observations, the difference could be due to the approximation of the uniform medium especially at large hypocentral distances. Increase in Q(C) with lapse time can be explained as the result of the depth dependent attenuation properties and multiple scattering effect.

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