2010
DOI: 10.1029/2009jb006955
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Synthesis of vector wave envelopes on the free surface of a random medium for the vertical incidence of a plane wavelet based on the Markov approximation

Abstract: [1] In short-period seismograms of earthquakes, we often observe the broadening of apparent duration of P and/or S waves and the excitation of the transverse component especially for P waves as travel distance increases. Such phenomena are well explained by scattering caused by random velocity fluctuation in the lithosphere. The Markov approximation is known as one of the powerful stochastic methods for the direct synthesis of wave envelopes. We extend the method to synthesize vector wave envelopes on the free… Show more

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Cited by 24 publications
(19 citation statements)
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“…Emoto et al (2010) examined how the free surface affects the wave envelope of each vector component after the propagation through a random medium for the vertical incidence of a plane wavelet. Emoto et al (2010) examined how the free surface affects the wave envelope of each vector component after the propagation through a random medium for the vertical incidence of a plane wavelet.…”
Section: Envelopes On the Free Surfacementioning
confidence: 99%
See 1 more Smart Citation
“…Emoto et al (2010) examined how the free surface affects the wave envelope of each vector component after the propagation through a random medium for the vertical incidence of a plane wavelet. Emoto et al (2010) examined how the free surface affects the wave envelope of each vector component after the propagation through a random medium for the vertical incidence of a plane wavelet.…”
Section: Envelopes On the Free Surfacementioning
confidence: 99%
“…Emoto et al (2010) examined how the free surface affects the wave envelope of each vector component after the propagation through a random medium for the vertical incidence of a plane wavelet. Emoto et al (2010) made a comparison of Markov envelopes and FD envelopes on the free surface of random media. In this case, multiplying the free-surface amplification factor for plane waves, which includes conversion between P-and S-waves, by the angular spectrum just beneath the free surface, and integrating it over ray angles, they calculate each displacement vector-component envelope on the free surface, where the excitation of surface waves is neglected.…”
Section: Envelopes On the Free Surfacementioning
confidence: 99%
“…(4) with C = 1 is valid for the full space. Because most stations are deployed on the surface, a free surface correction is introduced with a factor C = 4 (Emoto et al 2010). f can usually be approximated by the difference between upper and lower corner frequency depending on the filter design.…”
Section: O D E L E D a N D O B S E Rv E D E N E Rg Y D E N S I T I E Smentioning
confidence: 99%
“…The planewave incidence uses a solution of the up-going wave of the 1D wave equation in a homogeneous medium as an initial condition of the velocity and stress components at the bottom of the model (e.g., Emoto et al 2010). A bell-like-shaped spatial distribution corresponding to the source time function (Fig.…”
Section: Seismic Source Representationmentioning
confidence: 99%
“…The numerical simulation of seismic wave propagation is a fundamental tool for seismological studies such as estimation of the heterogeneous velocity structure (e.g., Tape et al 2009;Chen and Lee 2015), the study of seismic source processes (e.g., Lee et al 2006;Imperatori and Gallovič 2017), wave propagation in the heterogeneous Earth (e.g., Frankel and Clayton 1986;Emoto et al 2010) and hazard assessment (e.g., Graves et al 2010;Maeda et al 2016). Significant improvements in numerical simulation techniques, high-resolution velocity structure models and high-performance computer systems have enabled the use of 3D numerical simulations as a practical tool for regular data processing studies with currently available parallel computers.…”
Section: Introductionmentioning
confidence: 99%