scholarly journals Apparent attenuation by opto-acoustic defocus in phonon microscopy

2020 ◽  
Vol 19 ◽  
pp. 100180 ◽  
Author(s):  
Fernando Pérez-Cota ◽  
Salvatore La Cavera III ◽  
Shakila Naznin ◽  
Rafael Fuentes-Domínguez ◽  
Richard J. Smith ◽  
...  
Keyword(s):  
Solid Earth ◽  
2020 ◽  
Vol 11 (1) ◽  
pp. 161-171
Author(s):  
Susini deSilva ◽  
Vernon F. Cormier

Abstract. The relative contributions of scattering and viscoelastic attenuation to the apparent attenuation of seismic body waves are estimated from synthetic and observed S waves multiply reflected from Earth's surface and the core–mantle boundary. The synthetic seismograms include the effects of viscoelasticity and scattering from small-scale heterogeneity predicted from both global tomography and from thermodynamic models of mantle heterogeneity that have been verified from amplitude coherence measurements of body waves observed at dense arrays. Assuming thermodynamic models provide an estimate of the maximum plausible power of heterogeneity measured by elastic velocity and density fluctuations, we predict a maximum scattering contribution of 43 % to the total measured attenuation of mantle S waves having a dominant frequency of 0.05 Hz. The contributions of scattering in the upper and lower mantle to the total apparent attenuation are estimated to be roughly equal. The relative strength of the coda surrounding observed ScSn waves from deep focus earthquakes is not consistent with a mantle having zero intrinsic attenuation.


Geophysics ◽  
1987 ◽  
Vol 52 (1) ◽  
pp. 72-87 ◽  
Author(s):  
R. S. Jacobson

Despite many attenuation measurements which indicate a linear functional frequency dependence of absorption or constant [Formula: see text] in sediments, several theories predict no such linear dependence. The primary justification for rejecting a first‐power frequency dependence of attenuation is that it implies that seismic waves cannot propagate causally. Seismic waves must also travel with some velocity dispersion to satisfy causality, yet there is a lack of velocity dispersion measurements in sediments. In‐situ attenuation is caused by two distinct mechanisms: anelastic heating, and scattering due to interbed multiples. Apparent, or scattering, attenuation can produce both frequency‐dependent and non‐frequency‐dependent effects. Accurate measurements of attenuation and velocity dispersion are difficult; it is not surprising that a systematic investigation into the frequency dependence of absorption and velocity has not been made. A reinvestigation into two seismic refraction data sets collected over thickly stratified deep‐sea fans indicates that [Formula: see text] should not be assumed to be independent of frequency. Further, significant frequency‐independent absorption is present, indicating a high degree of apparent attenuation. Phase, or velocity, dispersion was also measured, but the results are more ambiguous than those for attenuation, due to inherent limitations of digital signals. Nevertheless, the absorption and velocity dispersion results are largely compatible, suggesting that if apparent attenuation is observed, then the scattered waves propagate causally.


2005 ◽  
Author(s):  
Ueyn L. Block ◽  
Vinayak Dangui ◽  
Michel J. F. Digonnet ◽  
Martin M. Fejer

Geophysics ◽  
1995 ◽  
Vol 60 (6) ◽  
pp. 1646-1655 ◽  
Author(s):  
Mark S. Sams

Layering that is finer than that typically resolved by sonic logging will contribute to apparent attenuation and anisotropy in the sonic‐to‐seismic frequency range. The significance of this contribution can be discerned through resolution enhancement of sonic and density logs. In this study a borehole compensated sonic and density log recorded in a cyclical sedimentary sequence have been enhanced by response matching with a high‐resolution microresistivity log. The additional resolved layering increases the layer‐induced dispersion by 50%, with the additional attenuation showing a peak with a Q of 135 at 1.2 kHz. The increase in average anisotropy is frequency dependent with a minimum increase of 50% at zero frequency. In the absence of high‐resolution data, the effects of layering can be severely underestimated, resulting in poor estimates of the intrinsic properties of rocks and their pore fluids.


2016 ◽  
Vol 16 (04) ◽  
pp. 1650009
Author(s):  
Josselin Garnier ◽  
Knut Sølna

Waves propagating through heterogeneous media experience scattering that can convert a coherent pulse into small incoherent fluctuations. This may appear as attenuation for the transmitted front pulse. The classic O’Doherty–Anstey theory describes such a transformation for scalar waves in finely layered media. Recent observations for seismic waves in the earth suggest that this theory can explain a significant component of seismic attenuation. An important question to answer is then how the O’Doherty–Anstey theory generalizes to seismic waves when several wave modes, possibly with the same velocity, interact. An important aspect of the O’Doherty–Anstey theory is the statistical stability property, which means that the transmitted front pulse is actually deterministic and depends only on the statistics of the medium but not on the particular medium realization when the medium is modeled as a random process. It is shown in this paper that this property generalizes in the case of elastic waves in a nontrivial way: the energy of the transmitted front pulse, but not the pulse shape itself, is statistically stable. This result is based on a separation of scales technique and a diffusion-approximation theorem that characterize the transmitted front pulse as the solution of a stochastic partial differential equation driven by two Brownian motions.


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