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64th EAGE Conference & Exhibition
- Conference date: 27 May 2002 - 30 May 2002
- Location: Florence, Italy
- Published: 27 May 2002
41 - 60 of 688 results
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Common Reflection Angle Migration
Authors Z. Koren, S. Xu and D. KosloffA-33 COMMON REFLECTION ANGLE MIGRATION Summary 1 We present a 2-D and 3-D ray-based migration/inversion approach for the construction of common image gathers (CIG) in the reflection angle domain. Amplitudes and phases of the reflected events are preserved for a wide range of angles even in complex areas with multi-arrivals. The method can be used for detailed velocity-model determination and for accurate amplitude variation with angle (AVA) analysis in such areas. Our method is a target-oriented approach based on shooting rays from the image points up to the surface. The method can also be applied as a model-based approach by
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Fresnel-Aperture PSDM
Authors H. Tabti and L.-J. GeliusA-34 FRESNEL-APERTURE PSDM Abstract 1 We introduce the Fresnel aperture which is the direct time-domain equivalent at the receivers’ surface of the subsurface Fresnel zone. Based on this concept we propose a new and efficient method for optimal aperture selection and Kirchhoff prestack depth migration. The problem with complex media is that multiple Fresnel apertures apparently exist for a given image point with just one of these corresponding to a possible real geological structure. Hence the contribution from these ‘false’ Fresnel apertures cause a noise-corrupted image of the subsurface. We propose a method by analogy with the velocity analysis where
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Computing Kirchhoff Depth Migration Traveltime from a Monofrequency Wavefield
By J.W. WigginsAbstract 1 A-35 COMPUTING KIRCHHOFF DEPTH MIGRATION TRAVELTIME FROM A MONOFREQUENCY WAVEFIELD WENDELL WIGGINS Prestack depth migration with the Kirchhoff-summation method requires maps of the wave traveltime from each source and receiver location to every image point. These traveltimes are usually computed by ray tracing or a finite-difference solution of the eikonal equation. Either of these methods gives the traveltime at an infinite frequency. In complex structures where the wave at any point is the sum over many slightly different diffracted paths the infinitefrequency times may not produce an ideal result because they do not model the diffraction and recombination
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Ray-Based Anti-Aliasing for Depth Migration
Authors S. Nguyen, R. Baina, M. Noble and P. ThierryA-36 RAY-BASED ANTI-ALIASING FOR DEPTH MIGRATION S.NGUYEN 1 R. BAINA 2 M. NOBLE 1 and P. THIERRY 1 Abstract 1 Operator/Imaging aliasing introduced in Kirchhoff migration is often tackled by trace tapering aperture truncation or a time and offset-variant filtering. The latter being the most suitable. However most implementations and published results using this technique are derived for Kirchhoff time migration and assume a constant velocity media. In this paper we introduce an anti-aliasing filter for ray-based pre-stack depth migration and valid for heterogeneous velocity models. We illustrate the benefits of such a scheme on a numerical and a real
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Aliasing in Wavefield Extrapolation Prestack Migration
More LessA-37 ALIASING IN WAVEFIELD EXTRAPOLATION PRESTACK MIGRATION YU ZHANG 1 JAMES SUN 1 and SAMUEL H. GRAY 2 Introduction 1 Aliasing during migration (“operator aliasing”) is widely recognized as a problem for Kirchhoff migration. It occurs when high-frequency reflection data are swept out at steep angles with the problem being worst for very coarse input trace spacing. The problem can be solved either by data interpolation to a finer-spaced grid of input traces or more commonly by anti-aliasing the migration operator (Gray 1992; Lumley et al. 1994; Abma et al. 2000; Biondi 2001 Zhang et al. 2001a). For two-dimensional (2-D)
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How to Choose a Subset of Frequencies for Frequency-Domain Finite-Difference Migration
Authors R-E. Plessix and W.A. MulderA-38 HOW TO CHOOSE A SUBSET OF FREQUENCIES FOR FREQUENCY-DOMAIN FINITE-DIFFERENCE MIGRATION R.-E. PLESSIX and W.A. MULDER Abstract 1 Frequency-domain finite-difference migration can be accelerated by an order of magnitude if a subset of the available data frequencies is used. To avoid unwanted artefacts the choice of this subset should be guided by two principles: sufficient localisation of reflectors and the avoidance of wrap-around. The first is related to the spatial resolution and Heisenberg’s principle. The second is needed to avoid repetitive patterns and is related to the Nyquist sampling theorem. Here we study both by a simple analytical and
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3D Prestack GSP Migration with Application to a Carbonate Data
Authors S. Jin and J. PajchelA-39 3D PRESTACK GSP MIGRATION WITH APPLICATION TO A CARBONATE DATA 1 EAGE 64 th Conference & Exhibition — Florence Italy 27 - 30 May 2002 1 1 SHENGWEN JIN Summary The generalized screen propagator (GSP) is a one -way wave equation based wide -angle propagator. GSP migration has been applied to both 2-D and 3-D prestack depth migrations for imaging complex velocity structures. Common azimuth offset domain GSP migration is an efficient 3-D prestack wavefield extrapolation algorithm based on double square root (DSR) equation and a stationary-phase approximation for the narrow azimuth nature of marine streamer data. Combined with
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Improving Near-Salt-Flank Imaging with Shot-Profile Wavefield-Extrapolation Migration in the Gulf of Mexico
Authors U.K. Albertin, D. Watts, W. Chang, S.J. Kapoor, C. Stork, P. Kitchenside and D. Yingst1 A-41 IMPROVING NEAR-SALT-FLANK IMAGING WITH SHOT-PROFILE WAVEFIELD- EXTRAPOLATION MIGRATION IN THE GULF OF MEXICO UWE ALBERTIN DAVE WATTS WENFONG CHANG S. JERRY KAPOOR Abstract Prestack Kirchhoff migration is widely used for imaging in complex areas and has been particularly effective in salt and subsalt imaging in the Gulf of Mexico. Despite this success there are areas where Kirchoff migration has difficulty imaging subsalt events. These difficulties are observed near salt flanks and under rugose salt bodies where migration artifacts often obscure primary sediment events. Among the causes for these artifacts are Kirchhoff’s use of a single traveltime arrival approximate
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3D Multi-Arrival Kirchhoff vs. Wave Equation Migration - SEG/EAGE Salt Model Case Study
Authors B. Duquet, G. Lambaré and S. XuA-42 3D MULTI-ARRIVAL KIRCHHOFF VS. WAVE EQUATION MIGRATION - SEG/EAGE SALT MODEL CASE STUDY G. LAMBARE 1 B. DUQUET 2 and S. XU 1 3 1 Abstract In the context of the SEG/EAGE Salt model experiment we compare results obtained by 3D multi-arrival preserved amplitude ray based migration with those obtained by 3D wave equation migration. The same dataset is used but both preprocessing and velocity model differ (for Kirchhoff migration some smoothing had to be applied to the exact velocity model). By the end the better quality of images obtained using wave equation migration with the exact velocity model
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Comparison of Kirchhoff and Wave-Equation Pre-Stack Migration on OBC Data
By R. Soubaras� � �ÇÅÈ�ÊÁËÇÆ Ç� ÃÁÊ�ÀÀÇ�� �Æ� Ï�Î� �ÉÍ�ÌÁÇÆ ÈÊ� ËÌ��à ÅÁ�Ê�ÌÁÇÆ ÇÆ Ç�� ��Ì� ËÙÑÑ�ÖÝ ÊÇ��ÊÌ ËÇÍ��Ê�Ë ��� ÖÙ� Ä��ÓÒ Å���ÙÜ � � Å�××Ý �Ö�Ò � Ì�� Ö� �ÒØ ���×���Ð�ØÝ Ó� ÔÖ� ×Ø� �Û�Ú� �ÕÙ�Ø�ÓÒ Ñ��Ö�Ø�ÓÒ �ÜÔÐ��Ò× Ø�� Ö�Ò�Û�Ð Ó� �ÒØ�Ö�×Ø �Ò Ø��× Ø� �Ò�ÕÙ� Ì��× Ô�Ô�Ö ¬Ö×Ø ��× Ù×× Ø�� ��Ú�ÒØ���× �Ò� �Ö�Û�� �× Ó� Ø�� ��«�Ö�ÒØ �ÜØÖ�ÔÓÐ�Ø�ÓÒ × ��Ñ�× �Ú��Ð��Ð� �ÓÖ Û�Ú� �ÕÙ�Ø�ÓÒ Ñ��Ö�Ø�ÓÒ Ì�� ÕÙ�×Ø�ÓÒ Ó� Û��Ø ØÓ �ÜÔ� Ø �ÖÓÑ � Û�Ú� �ÕÙ�Ø�ÓÒ Ñ��Ö�Ø�ÓÒ ÓÑÔ�Ö�� ØÓ � Ã�Ö ��Ó« ÓÒ� �× Ø��Ò ��Ö�××�� ��×�� ÓÒ � ×ÝÒØ��Ø� �Ò� � Ö��Ð ��Ø� �Ü�ÑÔÐ� ��Ò�ÐÐÝ Ø�� ÔÓ××���Ð�ØÝ Ó�
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Imaging under Complex Salt Bodies with 3D Prestack Finite Difference Depth Migration
Authors Z. Zhou, M. Guo and J.A. SteinA-44 Imaging under complex salt bodies with 3-D prestack finite difference depth migration Summary 1 We present an implicit finite difference depth migration (IFDM) system. Conventional aspects of IFDM are combined to produce a highly accurate downward continuation process. Appropriate imaging and aperture conditions are employed in a shot migration scheme to generate migrated image gathers in the shot-receiver offset domain. A highly efficient parallel implementation has been achieved without sacrificing accuracy. Results are obtained from both standard and in-house datasets from the SEG/EAGE 3-D Salt Model. These results along with real data examples demonstrate the high-quality sub-salt images obtainable
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Prestack Phase-Shift Migration of Separate Offsets in Laterally Inhomogeneous Media
More LessA-45 PRESTACK PHASE-SHIFT MIGRATION OF SEPARATE OFFSETS IN LATERALLY INHOMOGENEOUS MEDIA TARIQ ALKHALIFAH Summary 1 Using the stationary-phase method prestack phase-shift migration is implemented one offset at a time. This separate-offset implementation allows for a Fourier (reasonably fast) wave-equation type migration on data with irregular offset sampling. However the separate-offset phase-shift migration like its zero-offset counterpart handles only vertically inhomogeneous media. Using the combination of the split-step and the phase-shift-plusinterpolation (PSPI) approaches the separate-offset phase-shift migration is extended to handle laterally inhomogeneous media. Like any PSPI-based method the cost of the new migration relies heavily on the complexity of the
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Removing Distortions Caused by Water Velocity Variations - Method for Dynamic Correction
More LessB-01 REMOVING DISTORTIONS CAUSED BY WATER VELOCITY VARIATIONS - METHOD FOR DYNAMIC CORRECTION SCOTT MACKAY and JONATHAN FRIED 1 WesternGeco 1625 Broadway Suite 1300 Denver CO 80222 USA Summary Physical changes in ocean properties may occur during marine acquisition that can cause variations in water velocity. The result is a dynamic difference in traveltimes between overlapping infill data acquired at a later date. Such timing discrepancies may prevent accurate merging and imaging of the data. Unfortunately classical wave-equation solutions to this problem are typically impractical for 3D marine geometries. We present an approximate version of wave-equation layer replacement that addresses
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P-Wave and C-Wave Velocity Analysis for Deep Water OBC Data
Authors W. Wang Inc. and L.D. PhamB-02 P-WAVE AND C-WAVE VELOCITY ANALYSIS FOR DEEP WATER OBC DATA WEIZHONG WANG and LONG DON PHAM Summary 1 Deep-water OBC data are collected with sources and receivers at different depths. Seismic velocity estimation algorithms commonly used in processing assume that sources and receiver are at the same datum. To satisfy this requirement vertical shifts are applied to the data or straight ray projections are performed to bring shots and receivers to the same datum. If the sampling of the acquisition geometry is adequate then wave-equation datuming can also be applied. In this paper we present formulae for Pwave and
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Stacking Velocity Analysis with CRS Stack Attributes
Authors S. Bergler, P. Chira, J. Mann, K. Vieth and P. HubralB-03 STACKING VELOCITY ANALYSIS WITH CRS STACK ATTRIBUTES S. BERGLER P. CHIRA J. MANN K. VIETH and P. HUBRAL Geophysical Institute University of Karlsruhe Hertzstr. 16 76187 Karlsruhe Germany Abstract The Common-Reflection-Surface (CRS) Stack has been established over the past years as an alternative to standard data-driven imaging techniques. The CRS Stack not only yields high-quality stack sections from multi-coverage reflection pre-stack data but also provides—as by-product to the stacked section— important wavefield attributes. With the knowledge of the near-surface velocity only these attributes can be extracted from the stacking parameters which constitute the Common-Reflection-Surface stacking operator. The wavefield attributes
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Calibration of Depth Imaged Seismic Data Using an Interval Velocity Scaling Method
Authors A.A. Curtis, D.D. Stoughton, D.R. Hill, J.F. Ratcliffe and T. HartnettB-04 CALIBRATION OF DEPTH IMAGED SEISMIC DATA USING AN INTERVAL VELOCITY SCALING METHOD Summary 1 A. A. CURTIS D. D. STOUGHTON D. R. HILL J. F. RATCLIFFE and T. HARTNETT BHP Billiton Petroleum 1360 Post Oak Boulevard Houston TX 77056 USA As a consequence of anisotropy and other imaging effects horizon markers extracted from 3D seismic amplitude data frequently do not tie the equivalent formation intersections determined from well data. Such mis-ties between the seismic and well-log based formation markers can be quite significant in many Gulf of Mexico fields and are likely to be present in any 3D depth
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Pre Conditioning of the Densely Sampled Stacking Velocity Field
Authors D. Le Meur and P. HerrmannB-05 PRE CONDITIONING OF THE DENSELY SAMPLED STACKING VELOCITY FIELD Abstract 1 Over the last few years efficient methods have been developed to estimate densely sampled stacking velocity fields with the aim to improve the S/N ratio the spatial resolution and the frequency content of the stack. As a by-product this densely sampled attribute cube also becomes open to interpretation. The raw estimate of the automatically derived attribute is however too ‘noisy’ for immediate use. Fortunately the dense spatial and temporal sampling allows the use of efficient pre conditioning steps with a clear impact on the NMO stack result. Introduction
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The Key Practical Aspects of 3D Tomography - Data Picking and Model Representation
Authors F.J. Billette, J.T. Etgen and W.E. RietveldB-06 THE KEY PRACTICAL ASPECTS OF 3D TOMOGRAPHY - DATA PICKING AND MODEL REPRESENTATION Abstract 1 There are a wide variety of approaches to building velocity models with prestack depth migration. The most common pitfalls we see in them are extracting reliable yet detailed information about velocity errors from migrated data and then the inability to produce geologically reasonable velocity models from these error estimates. We extract detailed error estimates along horizons from finely sampled migrated data edit them statistically and QC the edits in map view. Tomography converts these error estimates into new velocity models or velocity model updates
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Model-Driven Data Interpolation vs. Velocity Knowledge Uncertainties
Authors P. Mazzucchelli, N. Bienati and U. SpagnoliniB-07 Model-driven data interpolation vs. velocity knowledge uncertainties. P. MAZZUCCHELLI 1 N. BIENATI 2 U. SPAGNOLINI 1 Abstract 1 Model-driven data interpolation performed by continuation algorithms (i.e. 3D SMO – Shot MoveOut) exploits the redundancy of the prestack data to regularize/densify survey geometries. Their usual Kirchhoff-type kernel implies that the accuracy of interpolation results is directly linked to the coverage of the operator itself [2] then coverage must be properly defined. A simple scalar index (e.g. fold of coverage) is not enough as it does not account for uneven dip illumination. Moreover the sensitivity of the continuation operators to velocity
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3D Stereotomographic Inversion on Real Data Set
Authors E. Chalard, P. Podvin, S. Le Bégat, P. Berthet and B. DavidB-08 3D STEREOTOMOGRAPHIC INVERSION ON REAL DATA SET Abstract 1 EMANUEL CHALARD 1 3 PASCAL PODVIN 1 SOAZIG LE BEGAT 1 PHILIPPE BERTHET 2 BERNARD DAVID 3 Stereotomography is a new tomographic method introduced in 2D by Billette and Lambaré (1998). It uses the apparent slopes of locally coherent seismic events picked in the prestack data cube to constrain the velocity model. In previous papers (Chalard et al. 2000a 2000b) we introduced the extension of stereotomography to 3D. In particular we proved that in the case of multi-streamer marine data acquisition the picking of seismic events can be performed independently
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