2008
DOI: 10.1190/1.2976118
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Passive seismic interferometry by multidimensional deconvolution

Abstract: We introduce seismic interferometry of passive data by multidimensional deconvolution ͑MDD͒ as an alternative to the crosscorrelation method. Interferometry by MDD has the potential to correct for the effects of source irregularity, assuming the first arrival can be separated from the full response. MDD applications can range from reservoir imaging using microseismicity to crustal imaging with teleseismic data.

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Cited by 138 publications
(92 citation statements)
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“…On the other hand, the MDD method would treat the amplitudes of both upgoing ͑r2͒ and downgoing reflections ͑r1 and r3͒ more accurately and would give better results ͑Figure 6a͒. This happens because the MDD method is more robust with respect to the source distribution than the CC method as shown in Wapenaar et al ͑2008b͒.…”
Section: Imaging Results From Crosscorrelation and Multidimensional Dmentioning
confidence: 99%
See 1 more Smart Citation
“…On the other hand, the MDD method would treat the amplitudes of both upgoing ͑r2͒ and downgoing reflections ͑r1 and r3͒ more accurately and would give better results ͑Figure 6a͒. This happens because the MDD method is more robust with respect to the source distribution than the CC method as shown in Wapenaar et al ͑2008b͒.…”
Section: Imaging Results From Crosscorrelation and Multidimensional Dmentioning
confidence: 99%
“…Even though the results from the CC method normally are deconvolved for the source spectra after correlation and summation, this deconvolution might not be trivial. Furthermore, when source arrays are irregular, wave amplitudes and traveltimes retrieved by the MDD method better represent the true wavefield than those from the CC method: The amplitudes of the wavefield retrieved by the CC method differ from the true wavefield, and the integration of the crosscorrelation results from the irregular source array would result in lower signal-to-noise ratio of the retrieved results ͑e.g., Snieder et al, 2006;Mehta et al, 2008b;Wapenaar et al, 2008b͒. On the other hand, the MDD method has several constraints: ͑1͒ MDD requires receiver arrays and therefore cannot be applied to a single receiver configuration, ͑2͒ MDD tends to be more CPU intensive than the CC method by array operation, and ͑3͒ MDD possibly is unstable because the inversion problem may be ill-conditioned.…”
Section: Introductionmentioning
confidence: 99%
“…Several algorithms have been used in seismic interferometry to obtain the wavefield. These include cross correlation [e.g., Claerbout, 1968;Bakulin and Calvert, 2004], deconvolution [e.g., Trampert et al, 1993;Snieder and Şafak, 2006], cross coherence [e.g., Aki, 1957;Prieto et al, 2009], and multidimensional deconvolution [e.g., Wapenaar et al, 2008;Minato et al, 2011].…”
Section: Retrieval Of the Wavefield Between Receiversmentioning
confidence: 99%
“…Another method is introduced by Wapenaar et al ͑2008͒, who propose the use of multidimensional deconvolution ͑MDD͒ of separated passive wavefields. They show that, theoretically, MDD will solve the problem of irregular source strength and irregular amplitude.…”
Section: ͑2007͒mentioning
confidence: 99%