Source wavelet effects on the ISS internal multiple leading-order attenuation algorithm and its higher-order modification that accommodate issues that.

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Presentation transcript:

Source wavelet effects on the ISS internal multiple leading-order attenuation algorithm and its higher-order modification that accommodate issues that arise when treating internal multiples as subevents Hong Liang M-OSRP Annual Meeting May 2, 2013 1 1

Motivation Objective: predict the amplitude and phase of internal multiples, without damaging primaries. prerequisites: reference wave removal source wavelet deconvolution source and receiver deghosting free surface multiple removal enhance the capability of the algorithm: from attenuation to elimination heighten the inclusiveness of the algorithm

Motivation Objective: predict the amplitude and phase of internal multiples, without damaging primaries. prerequisites: reference wave removal source wavelet deconvolution source and receiver deghosting free surface multiple removal enhance the capability of the algorithm: from attenuation to elimination heighten the inclusiveness of the algorithm

Motivation Objective: predict the amplitude and phase of internal multiples, without damaging primaries. prerequisites: reference wave removal source wavelet deconvolution source and receiver deghosting free surface multiple removal enhance the capability of the algorithm: from attenuation to elimination heighten the inclusiveness of the algorithm

Outline A brief review of the ISS internal multiple leading-order attenuation algorithm and its higher-order modification Source wavelet effects on the leading-order attenuator and its higher-order modification Using exact source wavelet: 1D example and 1.5D example Using estimated source wavelet Summary

The ISS leading-order attenuation algorithm ISS internal multiple attenuation method: does not require a priori information about the subsurface predict exact time and approximate amplitude predict internal multiples at all depths at once prerequisites: source wavelet deconvolved, reference wave removed, deghosted and free surface multiple removed Araújo et al.,1994, SEG Expanded Abstracts Weglein et al., 1997, Geophysics

The ISS leading-order attenuator For a 1D earth and a normal incident plane wave :constant velocity migration of incident spike plane-wave data ensures and : Green’s function in the reference medium : perturbation operator : migrated data-like first-order approximation to

The ISS leading-order attenuator Data primary + multiple primary + multiple primary + multiple

Subevent construction of an internal multiple + - = primary

Modification of the leading-order attenuator When both primaries and internal multiples in the data themselves act as subevents, the leading-order attenuator produces not only first-order internal multiples, but also higher-order internal multiples and, at times, creates spurious events. The ISS anticipates the issues due to spurious events, and higher-order terms in the series can provide the resolution.

An IM subevent in the second integral primary internal multiple primary + - = Number of reflectors , and spurious event negative of spurious event Ma et al., 2012, M-OSRP report

An IM subevent in one of the outer integral (1) + - = primary internal multiple Number of reflectors

An IM subevent in one of the outer integral (2) + - = primary internal multiple Number of reflectors

An IM subevent in one of the outer integral (3) primary primary internal multiple + - = Number of reflectors , and spurious event negative of spurious event Liang et al., 2012, M-OSRP report

Modification of the leading-order attenuator Adding the further terms to the current leading-order attenuator provides a modified ISS internal multiple algorithm. The modification retains the strength of the original algorithm while accommodating both primaries and internal multiples in the input data. Original Modification

Prediction with source wavelet deconvolution

Prediction with source wavelet deconvolution

Outline A review of the ISS internal multiple leading-order attenuation algorithm and its higher-order modification Source wavelet effects on the leading-order attenuator and its higher-order modification Using exact source wavelet: 1D example and 1.5D example Using estimated source wavelet Summary

Model for 1D synthetic data generation

Input trace red: primaries blue: internal multiples

Actual multiples .vs. Prediction red: actual internal multiples blue: predicted internal multiple without source wavelet deconvolution

Actual multiples .vs. Prediction (normalized) red: actual internal multiples blue: predicted internal multiple without source wavelet deconvolution

Prediction with source wavelet deconvolution

Actual multiples .vs. Prediction with decon red: actual internal multiples blue: predicted internal multiple with source wavelet deconvolution

Spurious event .vs. Prediction with decon red in circle: actual spurious event blue in circle: predicted spurious event with source wavelet deconvolution

Actual multiples .vs. Prediction with decon top and bottom red: actual internal multiples top blue: (with deconvolution) bottom blue: (with deconvolution)

Outline A review of the ISS internal multiple leading-order attenuator and its modification Source wavelet effects on the leading-order attenuator and its higher-order modification Using exact source wavelet: 1D example and 1.5D example Using estimated source wavelet Summary

Model for 1.5D data modeling

Data after deconvolution primary Data Data after deconvolution

Multiple prediction without deconvolution primary Data Multiple prediction without deconvolution

Multiple prediction with deconvolution primary Data Multiple prediction with deconvolution

Multiple prediction without deconvolution Wiggle comparison I312 I31212 I323 Data Multiple prediction without deconvolution

Multiple prediction with deconvolution Wiggle comparison I312 I31212 I323 Data Multiple prediction with deconvolution

Zero-offset traces red: input data red: input data spurious event spurious event I31212 I31212 I323 I323 red: input data blue: multiple prediction without source wavelet deconvolution red: input data blue: multiple prediction with source wavelet deconvolution

Spurious event prediction without deconvolution Multiple prediction without deconvolution (D3) Spurious event prediction without deconvolution (-D5PIP)

Spurious event prediction with deconvolution Multiple prediction with deconvolution (D3) Spurious event prediction with deconvolution (-D5PIP)

Outline A review of the ISS internal multiple leading-order attenuation algorithm and its higher-order modification Source wavelet effects on the leading-order attenuator and its higher-order modification Using exact source wavelet: 1D example and 1.5D example Using estimated source wavelet Summary

Example of inaccurate wavelet estimation red: exact source wavelet blue: estimated source wavelet

Prediction with inaccurate wavelet deconvolution Multiple prediction (zero offset): red: exact source wavelet blue: estimated source wavelet Spurious event prediction (zero offset): red: exact source wavelet blue: estimated source wavelet

Wavelet estimation based on Green’s theorem red: exact source wavelet blue: estimated source wavelet Weglein and Secrest, 1990, Geophysics.

Prediction with accurate wavelet deconvolution Multiple prediction (zero offset): red: exact source wavelet blue: estimated source wavelet Spurious event prediction (zero offset): red: exact source wavelet blue: estimated source wavelet

Outline A review of the ISS internal multiple leading-order attenuation algorithm and its higher-order modification Source wavelet effects on the leading-order attenuator and its higher-order modification Using exact source wavelet: 1D example and 1.5D example Using estimated source wavelet Summary

Prediction with source wavelet deconvolution

Summary Source wavelet can affect the amplitude and shape of internal multiple and spurious event prediction. By including the source wavelet deconvolution, the amplitude and shape of the prediction can be improved. The accuracy of source wavelet is important, and it could be estimated using Green’s theorem method.

References Araújo, F. V., A. B. Weglein, P. M. Carvalho, and R. H. Stolt, 1994, Inverse scattering series for multiple attenuation: An example with surface and internal multiples: 64th Annual International Meeting, SEG, Expanded Abstracts, 1039–1041. Ma, C., H. Liang, and A. B. Weglein, 2012, Modifying the leading order ISS attenuator of first-order internal multiples to accommodate primaries and internal multiples: fundamental concept and theory, development, and examples exemplied when three reectors generate the data: M-OSRP 2011 Annual meeting. Liang, H., C. Ma, and A. B. Weglein, 2012, A further general modification of the leading-order ISS attenuator of first-order internal multiples to accommodate primaries and internal multiples when an arbitrary number of reectors generate the data: theory, development, and examples: M-OSRP 2011 Annual meeting. Weglein, A. B., F. A. Gasparotto, P. M. Carvalho, and R. H. Stolt, 1997, An inverse scattering series method for attenuating multiples in seismic reflection data: Geophysics, 62, 1975–1989. Weglein, A. B., and Secrest, B. G. 1990. Wavelet estimation for a multidimensional acoustic earth model. Geophysics, 55, 902-913.

Acknowledgement Schlumberger / WesternGeco Mission-Oriented Seismic Research Program (M-OSRP)