2017
DOI: 10.1190/geo2016-0191.1
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Efficient wave-mode separation in vertical transversely isotropic media

Abstract: Wave-mode separation can be achieved by projecting elastic wavefields onto mutually orthogonal polarization directions. In isotropic media, because the P-wave’s polarization vectors are consistent with wave vectors, the isotropic separation operators are represented by divergence and curl operators, which are easy to realize. In anisotropic media, polarization vectors deviate from wave vectors based on local anisotropic strength and separation operators lose their simplicity. Conventionally, anisotropic wave-m… Show more

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Cited by 16 publications
(8 citation statements)
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“…However, this method cannot handle overlapping events (Tang et al . 2016; Zhou and Wang ; Lu and Liu ), which we will demonstrate in the following numerical experiment. The elastic Poynting vectors can be expressed as (Červený ) si=τijvj,where i and j represent the x ‐ or z ‐component of the elastic Poynting vectors s , respectively, τij and vj are the stress tensor and particle velocity, respectively.…”
Section: Methodsmentioning
confidence: 75%
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“…However, this method cannot handle overlapping events (Tang et al . 2016; Zhou and Wang ; Lu and Liu ), which we will demonstrate in the following numerical experiment. The elastic Poynting vectors can be expressed as (Červený ) si=τijvj,where i and j represent the x ‐ or z ‐component of the elastic Poynting vectors s , respectively, τij and vj are the stress tensor and particle velocity, respectively.…”
Section: Methodsmentioning
confidence: 75%
“…() developed an efficient method to propagate and decouple the elastic waves using the low‐rank approximations for anisotropic media. Zhou and Wang () introduced efficient anisotropic separation operators that are performed by locally rotating wave vectors to the qP‐wave polarization directions. They first calculate the deviation angles between these two vectors, which are estimated using the Poynting vectors.…”
Section: Introductionmentioning
confidence: 99%
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“…In the Fourier domain, the expressions are given as follows (Yan and Sava, 2009): truerightqtruePleft=ikxux+ikzuz=iωv(trueux,trueuz)·false(sinν,cosνfalse)T,rightqtrueSleft=ikzux+ikxuz=iωv(trueux,trueuz)·false(cosν,sinνfalse)T,where qP and qS are the qP‐ and qSV‐wavefields in the wavenumber domain, respectively; ux and uz are the elastic vector wavefields in the wavenumber domain; k=false(kx,kzfalse) is the polarization vector; ν is the polarization angle; ω is the circular frequency; and v is the phase velocity. All algorithms based on the spatial derivatives are under the control of this equation, such as the divergence and curl operators in isotropic media (Aki and Richards, 1980) and the separation operators of Zhou and Wang (2017). Taking the partial derivative with respect to x or z in the space domain is equivalent to multiplying the wavefield by the spatial wavenumber in the wavenumber domain ...…”
Section: Methodsmentioning
confidence: 99%
“…In isotropic media, the polarization vector is consistent with the wave vector for the P‐wave. In the anisotropic case, the polarization direction can be obtained by rotating the wave vector (Zhou and Wang, 2017), and the deviation angle is a function of the ratio of P‐wave velocity to S‐wave velocity VP0/VS0, Thomsen parameter ε, δ and phase angle θ.…”
Section: Methodsmentioning
confidence: 99%