2014
DOI: 10.3997/2214-4609.20141090
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An Interferometry-Based, Subsurface-Domain Objective Function for Targeted Waveform Inversion

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Cited by 5 publications
(2 citation statements)
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“…By applying the methodology at each depth level in the subsurface and taking the response at zero time lag and zero space lag, an image with accurate amplitudes can be obtained without artefacts from internal multiple reflections Broggini et al 2014a;Behura et al 2014). By including non-zero lags, equivalent extended images can also be created (Vasconcelos & Rickett 2013), which can be useful input for migration velocity analysis (Sava & Vasconcelos 2011), reservoir characterization (De Bruin et al 1990;Thomson 2012) and novel schemes for nonlinear imaging (Fleury & Vasconcelos 2012;Ravasi & Curtis 2012) and waveform inversion (Vasconcelos et al 2014a). Alternatively, we can use the Marchenko equations to retrieve internal multiples at the acquisition level, which could then be adaptively subtracted from the recorded data .…”
Section: Introductionmentioning
confidence: 99%
“…By applying the methodology at each depth level in the subsurface and taking the response at zero time lag and zero space lag, an image with accurate amplitudes can be obtained without artefacts from internal multiple reflections Broggini et al 2014a;Behura et al 2014). By including non-zero lags, equivalent extended images can also be created (Vasconcelos & Rickett 2013), which can be useful input for migration velocity analysis (Sava & Vasconcelos 2011), reservoir characterization (De Bruin et al 1990;Thomson 2012) and novel schemes for nonlinear imaging (Fleury & Vasconcelos 2012;Ravasi & Curtis 2012) and waveform inversion (Vasconcelos et al 2014a). Alternatively, we can use the Marchenko equations to retrieve internal multiples at the acquisition level, which could then be adaptively subtracted from the recorded data .…”
Section: Introductionmentioning
confidence: 99%
“…The ability to separate upgoing from downgoing waves when VA data are opportunely injected along the receiver array is not limited to back propagation (or propagation backward in time): The downgoing component can be propagated downward (and the upgoing component upward) by injecting the full recorded VA data forward in time and interchanging the sign of equation 4 (Robertson and Chapman, 2000;van Manen et al, 2007;Amundsen and Robertsson, 2014;Vasconcelos et al, 2014;Ravasi et al, 2015c).…”
Section: Discussionmentioning
confidence: 99%