superresolution imaging with resonance scatterring gerard schuster, yunsong huang, and abdullah...
TRANSCRIPT
Superresolution Imaging with Resonance
ScatterringGerard Schuster, Yunsong Huang, and Abdullah
AlTheyabKing Abdullah University of Science and Technology
Question: Dx << l/2?Migration: Dx=lz/4L LSM: Dx=l/2 Non-Linear LSM: Dx<<l/2
7 km
Outline
Summary
Question: Dx << l/2?
Answer: Dx=l/(4N+2)
Synthetic Testsvs
Field Data Tests
vs
Primary Resolution and ZO MigrationWhere is the Scatterer?
T
l/2=DxWhere did this come from?
Where did this come from?
Where did this come from?
Q: How thick is primary donut?: A l/2 (one roundtip)
2nd-order multiple
Primary Resolution and ZO MigrationWhere is the Scatterer?
T
Resonance Resolution and ZO MigrationWhere is the Scatterer?
1st-order multiple
Assume two interfaces, where we know location of one.
?Q: How thick is 1st order donut?: A l/4 (two roundtips)
Where is the other?
Q: How thick is 2nd order donut?
: A l/6 (three roundtips)
Question: Dx << l/2?
Answer: Dx=l/(2N+2)
Outline
Summary
Question: Dx << l/2?
Answer: Dx=l/(4N+2)
Synthetic Testsvs
Field Data Tests
vs
1-Bounce Migration 3-Bounce Migration
1-Scatterer ModelAssume perfect natural multiple migration operator, isolated multiples
6-Scatterer Model1-Bounce Migration 3-Bounce Migration
0.7 km
Assume we know locationsOf outer ring of scatterers
Outline
Summary
Question: Dx << l/2?
Answer: Dx=l/(4N+2)
Synthetic Testsvs
Field Data Tests
vs
Top of Salt
P
sea floor
top of salt
Primary Migration MResonance Migration
Advantage: gain in vertical resolutionSuperresolution by Resonant Multiples
Disadvantage: short-offset data only
Summary
kx
kg + ks
Reconstructed Model Spectrum
Dx=l/(2N+2) N-bounce Resonance
vs
Slight change in scatterer position amplified arrival
time+Superresolution
kz
vs
Primary top of salt Resonance top of salt
kz
kx
kz1st-order resonant multiples
SummaryLimitations Limited range of resonance wavenumbers for specular reflections Resonance can be very weak
Separation of different orders of resonance