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Q-interface imaging based on match-filter Q estimation

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(1)

Bei Li, Yunyue Elita Li, and Jizhong Yang

18/9/2019

Q-interface imaging based on

National University of Singapore

Singapore Geophysics Project

(2)

• Introduction

Seismic intrinsic attenuation Q-interface imaging

• Methodology

Shifted forward Q filtering Piecewise linear regression

• Example

Synthetic layered model

• Conclusions

(3)

Seismic intrinsic attenuation

waveform

Intrinsic attenuation can cause both amplitude decay and phase distortion of seismic waveform. Smaller Q indicates higher attenuation.

(4)

Q model building

Q estimation Q model update

Q tomography

Data domain Image domain

Time domain

Frequency domain Centroid/peak frequency shift (e.g., Quan and Harris, 1997) Amplitude spectral ratio

(e.g. Johnston et al., 1979) Complex spectral ratio

(e.g., Cheng and Margrave, 2008) Amplitude spectral ratio (+minimum phase)

(e.g., Cheng and Margrave, 2012) Full waveform (e.g, Li et al, 2018)

Wavenumber domain

Local wavenumber shift (e.g., Chen et al., 2018) Amplitude spectral ratio (e.g., Shen et al., 2018)

Ray tracing Wave equation modeling (e.g., Reine et al., 2012)

(e.g., Dutta and Schuster, 2016)

Q Full Waveform Inversion (Q-FWI) Q-interface imaging

(e.g., Plessix et al., 2016; Wang et al., 2018) (Li et al., 2018; Lin et al., 2018)

High-resolution options:

: Angular frequency

: Vsicoacoustic amplitude : Acoustic amplitude

Amplitude decay Velocity dispersion

: Acoustic velocity

: Viscoacoustic velocity : Reference frequency

(5)

Q-interface imaging with

virtual Q reflections

T ime 0

v

Distance De pth

Simple layered model illustration

: virtual Q reflectivity

Challenge: Physical reflections caused by pure Q contrast is too hard to be separated;

Solution: Synthesizing the virtual Q-reflections.

: attenuated travel time (Cavalca and Fletcher, 2009)

: acoustic waveform : viscoacoustic waveform : travel time 1 Q 2 Q

(6)

0

v

Distance De pth 1 Q 2 Q T ime

Simple layered model illustration

Match-filter Q estimation:

Shifted forward Q filtering to deal with unknown reference frequency;

Derivation of Q-interface information:

Piecewise linear regression to avoid instability of 2nd-order differencing.

: virtual Q reflectivity : virtual Q reflection : attenuated travel time

(Cavalca and Fletcher, 2009)

: acoustic waveform

: viscoacoustic waveform

Key points

(7)

• Introduction

Seismic intrinsic attenuation Q-interface imaging

• Methodology

Shifted forward Q filtering Piecewise linear regression

• Example

Synthetic layered model

• Conclusions

(8)

Match-filter Q estimation: forward Q filtering

Ideally, we know the corresponding pair of :

*Invert for by matching forward-Q filtered acoustic waveform with the viscoacoustic waveform

: Acoustic waveform generated using

Forward Q filtering ( ) based on and

(9)

Practically, we do not know the corresponding to :

Step 1:

Step 2:

: dominant frequency

Match-filter Q estimation:

shifted

forward Q filtering

: modeled acoustic waveform using : shifted modeled waveform

matching the modeled waveform with viscoacoustic waveform by shifting ( );

matching the shifted waveform with viscoacoustic waveform by Forward Q filtering based on dominant frequency.

(10)

Shifted forward Q filtering

Changing reference frequency by shifting:

= 1000 Hz

= 25 Hz

Velocity dispersion

: Acoustic velocity

(11)

Piecewise linear regression

(inversion for turning positions and slopes based on inverted samples):

Forward operator:

e.g., three-piece linear composition: ;

Inversion:

linearization: precondition:

: vector form of

: piecewise linear function composer : turning position vector, e.g.,

: slope vector, e.g., : inverted samples : sampling operator

: hyperbolic penalty function (Li et al., Geophysics, 2016)

(12)

• Introduction

Seismic intrinsic attenuation Q-interface imaging

• Methodology

Shifted forward Q filtering Piecewise linear regression

• Example

Synthetic layered model

• Conclusions

(13)

Velocity and Q models

(14)

Modeled waveform

Viscoacoustic record Picked velocity reflectivity Modeled waveform

(15)

Step 1: dynamic time shifting

Regular view

Windowed normalized view

(16)

Step 2: forward Q filtering for

inversion

Regular view

Windowed normalized view

(17)

Waveform-fitting for

Inverted

(zero-offset gather)

Inverted

(18)

Piecewise linear regression (3 pieces)

Shot No. 51 (1200 m), trace No. 101 (1000 m)

(19)

Virtual Q reflections

Virtual Q reflections

(zero-offset gather) (near-offset common shot gather) Virtual Q reflections

(20)

Q interface image

Q-interface image

Vertical profile (1200 m)

Reference depth for low Q anomaly

Top

(21)

• Introduction

Seismic intrinsic attenuation Q-interface imaging

• Methodology

Shifted forward Q filtering Piecewise linear regression

• Example

Synthetic layered model

• Conclusions

(22)

1. Match-filter Q estimation based on

shifted forward Q filtering

is

able to utilize both amplitude and phase information without knowing

the reference frequency corresponding to the modeled acoustic

waveform.

2. Piecewise linear regression can help to

stably and accurately

derive interface information in the data domain, including the

Q-interface that is not co-located with strong velocity Q-interfaces.

3. Q-interface imaging using the

synthetic virtual Q reflections

can

image the top and bottom boundary of typical isolated low-Q anomaly

with superior resolution.

(23)

Altering reference frequency by shifting

*A forward Q filtering on using , can also be achieved by firstly shifting it by and then forward Q filtering on using .

(24)

Reference frequency for the aligned acoustic waveform

Problem: Finding the reference frequency that is corresponding to satisfying:

,

where, ,

Solution:

(1) Substitute and into above minimization:

(2) According to Parseval’s theorem, we can ignore the phase term and only integrate amplitude:

(25)

Reference frequency for the aligned acoustic waveform

(3) Taking derivative w.r.t. :

(4) Tylor Expansion of at :

(26)

Thank you!

References

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