PROCESSING FOR SUBSALT IMAGING: A NEW AND FIRST TWO WAY MIGRATION METHOD THAT AVOIDS ALL HIGH FREQUENCY ASYMPTOTIC ASSUMPTIONS AND IS EQUALLY EFFECTIVE.

Slides:



Advertisements
Similar presentations
The Asymptotic Ray Theory
Advertisements

Reflection and Refraction of Light
Multiple Removal with Local Plane Waves
Ray theory and scattering theory Ray concept is simple: energy travels between sources and receivers only along a “pencil-thin” path (perpendicular to.
Chapter 26 Geometrical Optics. Units of Chapter 26 The Reflection of Light Forming Images with a Plane Mirror Spherical Mirrors Ray Tracing and the Mirror.
Reverse-Time Migration
Wave-equation migration velocity analysis Paul Sava* Stanford University Biondo Biondi Stanford University Sergey Fomel UT Austin.
True Amplitude WEM arising from True Amplitude One-way Wave Equations Yu Zhang, GuanQuan Zhang and Norman Bleistein.
Light in a Newtonian view Chapter 16. Introducing: light Light is the most important source of information for humans Concept of light rays - there are.
Body Waves and Ray Theory
AGENDA Tuesday, April 30, :00 PM Welcome Reception – El Fortin Lawn Wednesday May 1, 2013 – San Gabriel Room 7:00 AM Continental Breakfast - outside.
Seismic reflection Ali K. Abdel-Fattah Geology Dept.,
1 Optical Diffraction Theory and Its Applications on Photonic Device Design.
1 Identifiability of Scatterers In Inverse Obstacle Scattering Jun Zou Department of Mathematics The Chinese University of Hong Kong
Tom Wilson, Department of Geology and Geography Environmental and Exploration Geophysics II tom.h.wilson Department of Geology.
Tom Wilson, Department of Geology and Geography Environmental and Exploration Geophysics II tom.h.wilson Department of Geology.
Tom Wilson, Department of Geology and Geography Environmental and Exploration Geophysics II tom.h.wilson Department of Geology.
Green’s theorem requires the wavefield P and its normal derivative P n on the measurement surface as the input. In marine exploration, an over/under cable.
The acoustic Green’s function in 3D is the impulsive point source response of an acoustic medium. It satisfies the 3-D Helmholtz equation in the frequency.
Geometrical Optics.
1.1 Seismic Interferometry Optical interferometry.
The acoustic Green’s function in 3D is the impulsive point source response of an acoustic medium. It satisfies the 3-D Helmholtz equation in the frequency.
Perturbation Approach to Derive Born Approximation, Frechet Derivative, and Migration Operator Bowen Guo.
Including headwaves in imaging and internal multiple attenuation theory Bogdan G. Nita Research Assistant Professor, Dept. of Physics University of Houston.
Annual Meeting and Technical Review
Fang Liu and Arthur Weglein Houston, Texas May 12th, 2006
AGENDA Wednesday, May 28, :30 AM Welcome, program goals, objectives and overall strategy: Tutorial on the inverse scattering series and Green’s theorem.
ABSTRACT –Basic Principles and applications
examining the problem and its resolution
Inverse scattering terms for laterally-varying media
Zero-Offset Data d = L o ò r ) ( g = d dr r ) ( g = d
Imaging conditions in depth migration algorithms
Arthur B. Weglein M-OSRP, University of Houston Oct 22nd, 2015
Yanglei Zou* and Arthur B. Weglein
Xinglu Lin* and Arthur B. Weglein
Multi-dimensional depth imaging without an adequate velocity model
I. Tutorial: ISS imaging
Fang Liu, Arthur B. Weglein, Kristopher A. Innanen, Bogdan G. Nita
M-OSRP 2006 Annual Meeting, June 6, 2007
Accommodating the source (and receiver) array in the ISS free-surface multiple elimination algorithm: impact on interfering or proximal primaries and multiples.
Haiyan Zhang and Arthur B. Weglein
Lasse Amundsen, Arne Reitan, and Børge Arntsen
Good afternoon everyone. My name is Jinlong Yang
Kristopher Innanen** and Arthur Weglein* *University of Houston
M-OSRP Objectives To address and solve prioritized seismic E&P challenges (isolated task sub-series, intrinsic and circumstantial nonlinearity, and purposeful.
Wave-Equation Migration Research at Los Alamos National Laboratory
Kristopher Innanen and Arthur Weglein University of Houston
Source wavelet effects on the ISS internal multiple leading-order attenuation algorithm and its higher-order modification that accommodate issues that.
Wavelet estimation from towed-streamer pressure measurement and its application to free surface multiple attenuation Zhiqiang Guo (UH, PGS) Arthur Weglein.
Green’s theorem preprocessing and multiple attenuation;
Initial asymptotic acoustic RTM imaging results for a salt model
Initial analysis and comparison of the wave equation and asymptotic prediction of a receiver experiment at depth for one-way propagating waves Chao Ma*,
Inverse scattering internal multiple elimination
A first step towards the P wave only modeling plan
Haiyan Zhang and Arthur B. Weglein
Direct horizontal image gathers without velocity or “ironing”
Some remarks on the leading order imaging series
Tutorial: ISS and ISS multiple removal
Adriana C. Ramírez and Arthur B. Weglein
Jingfeng Zhang and Arthur B. Weglein
Adriana Citlali Ramírez
Remarks on Green’s Theorem for seismic interferometry
Elastic Green's theorem preprocessing
Haiyan Zhang and Arthur B. Weglein
Prestack depth migration in angle-domain using beamlet decomposition:
The general output of the leading-order attenuator
Bogdan G. Nita *University of Houston M-OSRP Annual Meeting
Presentation transcript:

PROCESSING FOR SUBSALT IMAGING: A NEW AND FIRST TWO WAY MIGRATION METHOD THAT AVOIDS ALL HIGH FREQUENCY ASYMPTOTIC ASSUMPTIONS AND IS EQUALLY EFFECTIVE FOR ALL FREQUENCY COMPONENTS OF BROADBAND DATA Arthur B. Weglein M-OSRP, University of Houston Oct 23 rd, 2015

2 Migration was originally (and remains today) only meaningful for primaries

The original purpose of migration was to map an event on a time section in (x,t) to a point on a structure map.That is, to a point on a reflector in x,z That concept only has meaning for primaries. We will show that that remains the meaning of migration today. 3

4 Wave theory methods used to migrate seismic data have two components 1. A wave propagation component 2. An imaging condition

5

2D Claerbout III (Stolt migration) Data on measurement surface Fourier transform Data at depth Data at depth at t=0

Inverse Fourier transform Set x g =x s =x (x m =x; x h =0 ) original Stolt migration (Claerbout III) angle average plane wave reflection coefficient by summing over k h 2D Claerbout III (Stolt migration) Change of variables

8 Stolt extended (Claerbout III) migration retains k h information at depth z, D(km,kh,kz) and that provides the plane wave reflection coefficient at a specular reflector Stolt and collaborators further extended Claerbout III to provide a point reflectivity model that automatically images specular and non- specular reflections. The latter is only possible for extensions/generalizations of Claerbout III(not for Claerbout II)

9 Claerbout imaging II Claerbout imaging III

Let’s examine Claerbout II and III where only the imaging condition is the issue 10

Zou and Weglein,

12

13

The Claerbout II imaging principle provides an image for one shot record. However, the resulting inconsistency in the image is mitigated by summing over shots. Claerbout II has a somewhat ad hoc origin and an ad hoc ‘fix’.

In Claerbout III one shot record predicts the receiver at depth (not an image). The Green’s theorem weighted sum over shots then predicts the source at depth, leading to an image. There is nothing that’s inconsistent or being fixed with the sum over sources in Claerbout III.

How do you know if a migration method has made a high frequency approximation? 16

17 (1) If there is a travel time curve of candidate images within the method, it is a high frequency ‘ray theory’ approximation/ assumption. where,

18 Zou, 2015 Stolt migration: one source one receiver RTM(2D) z x Claerbout IIIClaerbout II No high frequency assumptionHigh frequency assumption Imaging Conditions and High Frequency Assumptions

How do you know if a migration method has made a high frequency approximation? (2) A stationary phase of other high frequency approximation is employed within the method. (3) a propagation model that assumes one way wave propagation (for anything other than a homogeneous subsurface) is a high frequency approximation high frequency approximation can enter migration methods through (1) the imaging condition (all Claerbout II) or (2) through the propagation component (or both), that is, for example, assuming a one way propagation for a slowly varying velocity in Claerbout III 19

20 An asymptotic approximation can be made with the stationary phase approximation 2D Stolt migration

The Kirchhoff migration is an asymptotic approximation of Stolt migration 21

Kirchhoff migration for a single source and receiver Kirchhoff migration (2D) x z Zou et al, High Frequency approximation from a stationary phase approximation

Claerbout II and III have been extended and generalized For Claerbout II e.g., Yu Zhang, Sheng Xu and Norman Bleistein introduce a geometric optics reflection coefficient model relating the reflection data and the incident source wavefield. For Claerbout III Stolt and collaborators non-zero offset at t=0 provides amplitude information outputs plane wave reflection coefficient or point scatterer reflectivity for specular and non-specular reflection 23

24

Zou and Weglein,

Benefits of Claerbout III imaging (extended by Stolt and colleagues) for specular and non-specular imaging 1. Specular outputs actual plane wave reflection coefficient data for specular reflection (unique to Claerbout III ) 2. Non-Specular reflection a point scatterer model for structure and inversion of non-specular reflections (unique to Claerbout III ) specular non-specular 26

27

M-OSRP has recently pioneered and developed a new migration method that has Stolt’s extension of Claerbout III imaging inside a medium with two way waves The new migration method provides four benefits 28

29 Recent new imaging development from M-OSRP (Weglein, A.B., Stolt, R. H., Mayhan, J. D., “Reverse-time migration and Green’s theorem: Part I — The evolution of concepts, and setting the stage for the new {RTM} method” Journal ofSeismic Exploration, 20, 73–90. February 2011; Weglein, A.B., Stolt, R. H., Mayhan, J. D., “Reverse time migration and Green’s theorem: Part II — A new and consistent theory that progresses and corrects current RTM concepts and methods” Journal ofSeismic Exploration, 20, 135–159. May 2011; THE FIRST WAVE EQUATION MIGRATION RTM WITH DATA CONSISTING OF PRIMARIES AND INTERNAL MULTIPLES: THEORY AND 1D EXAMPLES FANG LIU and ARTHUR B. WEGLEIN JOURNAL OF SEISMIC EXPLORATION 23, (2014) 357) provides the predicted source and receiver experiment at depth beneath an overburden that has two way wave propagation 1.A tool to analyze the role of primaries and multiples in imaging 2.A more effective and interpretable RTM by realizing Stolt extended Claerbout III providing a more complete realistic model for imaging and inverting specular and non-specular reflectors 3.Provides the first migration method for a smooth or discontinuous velocity that is equally effective at every frequency component of recorded data (avoids asymptotic high frequency approximations) in both the imaging condition and in how the imaging condition is implemented. 4.Imaging and inverting Claerbout III from above (and from below) a reflector without Claerbout II issues that the de-primary activity seeks to address (e.g., backscatter and other false images).

30 Use the new imaging method with two way propagating waves to examine the role of primaries and multiples in imaging and inversion That provides a definitive response to the question of whether multiples are migrated

31

32

33

34

35

36

37

38

39

40

A TWO-REFLECTOR MODEL 41 R1R1 R2R2 a1a1 a2a2 c1c1 c2c2 c3c3

42

43 Data at depth

44

SUMMARY We present the first migration method for imaging that is equally effective at all frequencies. 45

46