CN106338766A - Pre-stack time migration method based on split-step Fourier algorithm - Google Patents
Pre-stack time migration method based on split-step Fourier algorithm Download PDFInfo
- Publication number
- CN106338766A CN106338766A CN201510394531.8A CN201510394531A CN106338766A CN 106338766 A CN106338766 A CN 106338766A CN 201510394531 A CN201510394531 A CN 201510394531A CN 106338766 A CN106338766 A CN 106338766A
- Authority
- CN
- China
- Prior art keywords
- time
- imaging
- field
- split
- velocity
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Granted
Links
Landscapes
- Geophysics And Detection Of Objects (AREA)
Abstract
The invention provides a Pre-stack time migration method based on a split-step Fourier algorithm. The method comprises the steps of inputting pre-processed seismic data; picking up the root mean square speed in an interactive mode; calculating the ray propagation time from an imaging point to a focus point; converting seismic data of a time-space domain into frequency-wave number; acquiring a continuation value of a background wave field; transforming the continued wave field into the frequency-space domain through Fourier transform, and performing a time shift operation through a split-step Fourier time shift operator of the time domain so as to realize continuation for a disturbance wave field; and performing phase shift on a frequency-space domain seismic wave field and carrying out integration on the effective frequency band by using a excitation time imaging condition so as to acquire a seismic imaging result of a shot record. The pre-stack time migration method based on the split-step Fourier algorithm can carry out migration by applying the root mean square speed, and improves the adaptive capacity for speed vertical and longitudinal variations and the amplitude preserving capacity for migration imaging of pre-stack time migration under the condition of not increasing the speed modeling difficulty.
Description
Technical field
The present invention relates to the migration imaging field in seism processing, especially relate to a kind of being based on and divide
The prestack time migration method of step Fourier algorithm.
Background technology
Seismic migration is a kind of complementary operation that earthquake information enters rearrangement, to make seismic wave energy return
Position, to the actual position in its space, obtains underground real construction form.Wave equation prestack migration imaging master
It is divided into pre-stack time migration imaging and pre-stack depth migration imaging two class.Pre-stack depth migration is to underground speed
Degree cross directional variations strong adaptability, it is possible to provide the photo-quality imaging result of Depth Domain, but its essence to rate pattern
Degree has high demands and computationally intensive, therefore, is the scheme of a high investment high repayment.Pre-stack time migration becomes
As computational efficiency is high, its requirement to rate pattern application conditions is low simultaneously, horizontal in construction complexity, speed
There is preferable imaging effect in the case of change less.Therefore, pre-stack time migration is reality at this stage
Use technology.
Pre-stack time migration imaging can be divided into two big class according to the principle that algorithm is realized: based on ray theory
Offset method and the offset method based on wave field extrapolation.Conventional ray method pre-stack time migration adopts mean square
Root speed, it is capable of vertically and horizontally speed change, and amount of calculation is less, and calculates root mean sequare velocity and improve
Its precision comparison is easy, but its numerical value response characteristic is not so good as wave field method.Even so, current main flow
In seismic data processing software, pre-stack time migration (pstm) still only has ray method without wave field method.This
It is because that wave field method pstm quotes interval velocity in recursive process, during calculating, m- interval velocity model has very
Big difficulty.Therefore, in practice, if spending equal cost if necessary, people would rather set up depth
- interval velocity model the higher pre-stack depth migration of choice accuracy, so, quoting interval velocity model becomes
The biggest obstacle of wave field method pstm.
With the increase of oil-gas exploration difficulty, it is more and more important that seismic data protects width process.Go out in recent years
Show plane wave, phase shift adds interpolation and the wave field class prestack time migration technique such as constant-velocity scan, but it is all
Multi objective cannot meet real requirement.
In frequency wavenumber domain, dubrulle (1983), ekren and ursin (1999) achieve to common big gun
Inspection away from plane wave wave field extrapolation.But, common offset road collection plane wave pre-stack time migration in theory
Can process has vertical velocity change medium, and for Seismic Wave Dynamics Characteristics holding also need into
One step improves.
Integral formula (ehinger a., lailly p., and marfurt k.j. from single track Green's function
1996) set out, jianhua p. and dan n. (2008) borrows phase shift method and obtains responding spy with wave field method
The kirchhoff type pre-stack time migration result of property.This mode can retain the major advantage of ray method,
Amplitude and waveform characteristic can also be improved.But, carried out in units of road wave field extrapolation can lead to considerable
Amount of calculation.
Wang Youxin (2008) realizes the pre-stack time migration to single shot record by the method that phase shift adds interpolation.
The method imaging angle is high, but computationally intensive, calculates wave field by linear interpolation it is impossible to adapt to laterally
The large change of speed.
Sergey fomel (2013) proposes wave equation goes to from cartesian coordinate system imaging ray seat
The method being solved under mark system, The method avoids in Conventional Time skew to Green's function calculating
Approximate solution, improves time migration computational accuracy, but its cross directional variations bad adaptability to speed.
Because wave field method has good numerical characteristic, so, wave field method pre-stack time migration has important
Practical value, many research work attempt to the estimated performance of wave field method, but are limited by and quote all
Root speed and speed-adaptive change two problems it is difficult to meet real requirement.We have invented one for this
Plant the new prestack time migration method based on split-step fast fourier transformation, solve this two technical problems.
Content of the invention
It is an object of the invention to provide a kind of can produce more true and reliable imaging results based on point
The prestack time migration method of step Fourier algorithm.
The purpose of the present invention can be achieved by the following technical measures: the prestack based on split-step fast fourier transformation
Time migration method, should be included based on the prestack time migration method of split-step fast fourier transformation: step 1,
Input pretreated geological data pu(t,x,y);Step 2, using pretreated geological data
pu(t, x, y) is calculated root mean sequare velocity spectrum, picks up root mean sequare velocity by interactive mode, and obtains work
Mean-square-root velocity field v in the range of arearms(t,x,y);Step 3, based on mean-square-root velocity field vrms(t, x, y), meter
It is counted as picture point to the ray propagation time τ of focal point;Step 4, using Fourier transformation, by when m- sky
Between domain geological data pu(t, x, y) transforms to frequency wavenumber domain p* u(w,kx,ky), wherein,
p* u(w,kx,ky)=fft (pu(t,x,y));Step 5, using step Fourier phase-shift operator by p* u(w,kx,ky) straight
Connect continuation to the time τ of underground imaging point, obtain the continuation value of background wave field;Step 6, by continuation
Wave field afterwards is fourier transformed Frequency-Space Domain, by the step Fourier time-displacement operator of time domain
Carry out time shift computing, realize the continuation to disturbance wave field;And step 7, according to imaging point to focal point
Ray propagation time τ, using firing time image-forming condition, phase place is made to Frequency-Space Domain seismic wave field
Move and carry out the integration of effective frequency range, obtain the seismic imaging result of big gun record.
The purpose of the present invention also can be achieved by the following technical measures:
In step 1, interval velocity model in depth domain is just being drilled with the common big gun collection p obtainingu(t, x, y) carry out denoising,
These conventional pretreatment of static correction.
In step 2, pick up the root mean sequare velocity of seed point location by interactive mode, insert through three-dimensional
The smooth mean-square-root velocity field v obtaining target area of valuerms(t, x, y), described mean-square-root velocity field is used for earthquake
The step Fourier pre-stack time migration of data.
In step 2, using pretreated geological data pu(t, x, y) calculates root mean sequare velocity spectrum, passes through
Interactive mode, picks up the root mean sequare velocity of seed point location at equal intervals according to 100 meters, then passes through interpolation
Smooth acquisition is spaced apart the time domain mean-square-root velocity field v of 10 meters of modelrms(t, x, y), that is, prestack time is inclined
Move required velocity field.
In step 3, based on mean-square-root velocity field vrms(t, x, y), calculates imaging point using ray method and arrives
The ray propagation time of focal pointWherein, τ is the time of imaging point, and x is
The position of imaging point, xsFor the position of focal point, vrmsFor root mean sequare velocity.
In steps of 5, by the mean-square-root velocity field in application time domain, obtained by single step continuation,
The mutually transposition of background velocity is directed on continuation time τ, described phase-shift operator expression formula is as follows:
Wherein, vrms0(τ) for the background root-mean-square field speed angle value in τ moment, srms0(τ) for the slowness of ambient field,
And srms0(τ)=1/vrms0(τ), w is frequency, kxFor the wave number in x direction, kyWave number for y direction.
In step 6, calculated for step 5 wave field is transformed into frequency-space through Fourier inversion
Domain, on this basis by the step Fourier time-displacement operator of time domain be calculated for Perturbation when
Transposition, applies time-displacement operator, realizes the continuation to Perturbation, its expression formula is:
Wherein, δ srms(τ, x, y) is the slowness of Perturbation, so far, completes the earthquake of geophone station side is remembered
The wave field extrapolation in record τ moment at imaging point position.
In step 7, Frequency-Space Domain seismic wave field continuation value step 6 being obtained, during according to exciting
Between image-forming condition implementing phase mobile and effective frequency range is integrated, obtain final temporal-spatial field
Seismic wave field value, its image-forming condition expression formula is:
Wherein, i is the temporal-spatial field seismic wave field after phase shift, w1 to w2 having for seismic wave
Effect frequency band range.
Step 7 also includes: record-shifted for big gun imaging is converted into common imaging gather, merges identical big gun inspection
Away from;All single-shot imaging results are superimposed according to locus, or the direct superposition to common imaging gather,
Obtain the pre-stack time migration imaging results of target area.
The present invention proposes a kind of prestack time migration method based on split-step fast fourier transformation, key therein
It is that wave field extrapolation is realized according to root mean sequare velocity.Generally, ray method quotes root mean sequare velocity, and wave field method is drawn
With interval velocity, and set up interval velocity model and have great difficulty, so, pre-stack time migration is mainly using penetrating
Collimation method.However, the numerical value response characteristic of ray method pre-stack time migration is not so good as wave field method and guarantor's width is poor,
For this reason, it is pre-stack time migration needs that the application root mean sequare velocity being capable of simple and fast realizes the skew of wave field method
The major issue solving.In wave field class algorithm, phase shift method, plane wave method, step Fourier and
Screen algorithm can become progressively recursion into One-step Extrapolation, thus quoting root mean sequare velocity, wherein step Fourier
Algorithm is succinct and has single order lateral velocity variation ability, just meets the precondition of pre-stack time migration.This
Invention is based on split-step fast fourier transformation, and application root mean sequare velocity achieves wave field method pre-stack time migration, its
It is mainly characterized by: 1. quote root mean sequare velocity, speed is realized by single step wave field extrapolation longitudinally varying, keep away
Exempt from the error that interval velocity introduces in successively recursion downwards;2. compensated by relative time shift and realize laterally speed
Degree single order change;3. pass through the mixing of shot point ray method and geophone station wave field method, realize ray method high efficiency
Mutual supplement with each other's advantages with wave field method high-fidelity.Either ray method or wave field method, both can use in theory
In pre-stack time migration it is also possible to be used for pre-stack depth migration.In practice, if it is known that interval velocity, fold
Front depth migration is better than the imaging effect of pre-stack time migration, but, due to calculating accurate interval velocity ratio
Calculate root mean sequare velocity difficult, therefore, wave field method pre-stack time migration is realized not using mean-square-root velocity field
Lose as the high imaging method of a kind of efficient quick, fidelity.
The prestack time migration method based on split-step fast fourier transformation of the present invention, wave field method prestack time is inclined
Before moving technology application, first the pretreatment such as conventional denoising, static correction are carried out to geological data, by analysis
Geological data, obtains accurate mean-square-root velocity field.Then, using ray method, calculate focal point to becoming
The raytime of picture point.Now, geological data is transformed into frequency wavenumber domain, using background root-mean-square
The geological data of velocity on frequency-wave-number domain carries out a phase shift, realizes the wave field extrapolation to ambient field;
Geological data after continuation is transformed to Frequency-Space Domain, is carried out once using disturbance mean-square-root velocity field
Time shift, realizes the wave field extrapolation to Perturbation;According to the propagation time of focal point to imaging point, to continuation
Frequency-Space Domain wave field implementing phase afterwards moves;After moving through wavefield phase, to seismic wavefield data
Carry out the integration of effective frequency range, obtain final seismic wave field continuation value;Finally, all single-shots are imaged
Result is superimposed according to locus, or the direct superposition to common imaging gather, obtains the prestack of target area
Time migration imaging results.
Inexpensive root mean sequare velocity should be adopted by prestack time migration method based on split-step fast fourier transformation
Field achieves the pre-stack time migration based on split-step fast fourier transformation, avoids layer by single step wave field extrapolation
Speed repeats constantly positive inverse transformation in downward recursion, improves skew while not increasing and calculate cost
Precision simultaneously improves amplitude response.Meanwhile, by the hybrid operation of ray method and wave field method, both embodied
The good amplitude response of wave field method also adopts the advantage of ray method speed-adaptive change in time and space, takes
The effect that must have complementary advantages, is greatly improved computational efficiency.Compared with conventional pre-stack time migration algorithm,
The present invention can apply root mean sequare velocity to enter line displacement, in the case of the modeling difficulty that do not gather way, carries
Adaptability and the guarantor's width ability to migration imaging that high pre-stack time migration vertically and horizontally changes to speed.
Brief description
Fig. 1 is the specific embodiment of the prestack time migration method based on split-step fast fourier transformation of the present invention
Flow chart;
Fig. 2 is the corresponding depth of marmousi model-interval velocity schematic diagram in the specific embodiment of the present invention;
Fig. 3 be the present invention specific embodiment in marmousi model corresponding when m- root mean sequare velocity show
It is intended to;
Fig. 4 is the ray method pre-stack time migration result of marmousi model in the specific embodiment of the present invention
Schematic diagram;
Fig. 5 is the ripple based on split-step fast fourier transformation of marmousi model in the specific embodiment of the present invention
Field method pre-stack time migration result schematic diagram;
Specific embodiment
Purpose, technical scheme and advantage for enabling the embodiment of the present invention become apparent, below in conjunction with
Accompanying drawing in the embodiment of the present invention, carries out clear, complete retouching to the technical scheme in the embodiment of the present invention
State.
As shown in figure 1, Fig. 1 is the prestack time migration method based on split-step fast fourier transformation of the present invention
Flow chart.
In step 101, input geological data, this geological data is pre- through conventional denoising, static correction etc.
The common-shot-gather processing.In one embodiment, to marmousi Depth Domain interval velocity as shown in Figure 2
The common big gun collection p that forward modeling obtainsu(t, x, y) carries out the routine pretreatment such as denoising, static correction.Flow process enters
To step 102.
In step 102, pick up root mean sequare velocity, be calculated using pretreated geological data mean square
Root normal-moveout spectrum, picks up the root mean sequare velocity of seed point location by interactive mode, smooths through three-dimensional interpolation
Obtain the mean-square-root velocity field of target area, described mean-square-root velocity field is used in substep Fu of geological data
Leaf pre-stack time migration.In one embodiment, using pretreated geological data pu(t, x, y) calculates all
Root normal-moveout spectrum, by interactive mode, the root-mean-square picking up seed point location according to 100 meters at equal intervals is fast
Degree, then obtains the time of the as shown in Figure 3 marmousi model being spaced apart 10 meters by interpolation smoothing
Domain mean-square-root velocity field vrms(t, x, y), i.e. velocity field needed for pre-stack time migration.Flow process enters into step
103.
In step 103, when being travelled using ray computational methods and adopt described mean-square-root velocity field, calculate
Imaging point is to the ray propagation time of focal point.In one embodiment, based on mean-square-root velocity field
vrms(t, x, y), calculates imaging point to the ray propagation time of focal point using ray methodWherein, τ is the time of imaging point, and x is the position of imaging point, xsFor shake
The position of source point, vrmsFor root mean sequare velocity, flow process enters into step 104.
In step 104, using Fourier transformation, the common-shot-gather of temporal-spatial field is transformed to frequency
- wave-number domain.In one embodiment, changed by two-dimentional Fourier, by the geophone station side through pretreatment
Geological data is changed into the p of frequency wavenumber domain* u(w,kx,ky), wherein p* u(w,kx,ky)=fft (pu(t,x,y)).
Flow process enters into step 105.
In step 105, using step Fourier phase-shift operator and using described mean-square-root velocity field to described
Common-shot-gather geological data carries out wave field extrapolation, obtains the outer frequency wavenumber domain seismic wave number of fields postponing
According to.
To earthquake market demand one by reference background slowness srms0(τ) phase-shift operator obtaining.Deep in prestack
In degree skew, the step-length of phase shift continuation is a fixing depth value δ z, needs to obtain into by Layer by layer recurrence
The wave field extrapolation value of image point position.In embodiments of the present invention, by the root mean sequare velocity in application time domain
, obtained by single step continuation, the mutually transposition of background velocity, described phase shift are directed on continuation time τ
Operator expression formula is as follows:
Wherein, vrms0(τ) for the background root-mean-square field speed angle value in τ moment, srms0(τ) for the slowness of ambient field,
And srms0(τ)=1/vrms0(τ), w is frequency, kxFor the wave number in x direction, kyWave number for y direction.
Application above-mentioned formula is it is possible to by upgoing wave p* u(w,kx,ky) directly continuation is to underground imaging point
On time τ, obtain the continuation value of background wave field.Flow process enters into step 106.
In step 106, using Fourier inversion, by the frequency wavenumber domain postponing outward seismic wavefield data
Transform to Frequency-Space Domain, the Frequency-Space Domain seismic wavefield data after being converted.Using substep Fu
In leaf time-displacement operator and using described mean-square-root velocity field to conversion after Frequency-Space Domain seismic wave number of fields
According to carrying out continuation process, obtain the Frequency-Space Domain seismic wavefield data of secondary continuation.
Calculated for step 105 wave field is transformed into Frequency-Space Domain through Fourier inversion, in this base
On plinth, the when transposition for Perturbation, application are calculated by the step Fourier time-displacement operator of time domain
Time-displacement operator, realizes the continuation to Perturbation, its expression formula is:
Wherein, δ srms(τ, x, y) is the slowness of Perturbation.
So far, complete the wave field extrapolation to geophone station side earthquake record τ moment at imaging point position.
Flow process enters into step 107.
In step 107, according to the ray propagation time of described focal point to imaging point, using firing time
Image-forming condition, makees phase shift to Frequency-Space Domain seismic wave field and carries out the integration of effective frequency range, obtain
Seismic imaging result to big gun record;Record-shifted for big gun imaging is converted into common imaging gather, merges phase
Same geophone offset, this image gather can be used for later stage avo analysis and lithological inversion;All single-shots are become
As result is superimposed according to locus, or the direct superposition to common imaging gather, obtain the folded of target area
Front time migration imaging results.
In one embodiment, Frequency-Space Domain seismic wave field continuation value step 106 being obtained, according to sharp
Send out time image condition implementing phase to move and effective frequency range is integrated, obtain final when m- sky
Between domain seismic wave field value, its image-forming condition expression formula is:
Wherein, i is the temporal-spatial field seismic wave field after phase shift, w1 to w2 having for seismic wave
Effect frequency band range.
Picture value is become according to described final temporal-spatial field seismic wave field, by its all single-shot imaging results
According to locus superposition, or record-shifted for big gun imaging is converted into common imaging gather, to common imaging
Point road collection is directly superimposed, just can obtain step Fourier pre-stack time migration imaging knot as shown in Figure 5
Really, compared with the marmousi migration result being obtained using ray method pre-stack time migration shown in Fig. 4, adopt
Wave field abundant information in the migration result being obtained with the inventive method, the internal weak reflection in stratum is clear, embodies
Guarantor's width of wave field method migration before stack, simultaneously at position shown in square frame, is obtained using the inventive method
Fault imaging result improve a lot compared with ray method skew, breakpoint is clear-cut, and resolution is also higher.
Claims (9)
1. the prestack time migration method based on split-step fast fourier transformation is it is characterised in that this is based on
The prestack time migration method of split-step fast fourier transformation includes:
Step 1, inputs pretreated geological data pu(t,x,y);
Step 2, using pretreated geological data pu(t, x, y) is calculated root mean sequare velocity spectrum,
Root mean sequare velocity is picked up by interactive mode, and obtains mean-square-root velocity field in the range of work area
vrms(t,x,y);
Step 3, based on mean-square-root velocity field vrms(t, x, y), the ray calculating imaging point to focal point passes
τ between sowing time;
Step 4, using Fourier transformation, by the geological data p of temporal-spatial fieldu(t, x, y) transforms to
Frequency wavenumber domain p* u(w,kx,ky), wherein, p* u(w,kx,ky)=fft (pu(t,x,y));
Step 5, using step Fourier phase-shift operator by p* u(w,kx,ky) directly continuation arrive underground one-tenth
On the time τ of picture point, obtain the continuation value of background wave field;
Step 6, the wave field after continuation is fourier transformed Frequency-Space Domain, by time domain
Step Fourier time-displacement operator carries out time shift computing, realizes the continuation to disturbance wave field;And
Step 7, according to the ray propagation time τ of imaging point to focal point, using firing time imaging
Condition, makees phase shift to Frequency-Space Domain seismic wave field and carries out the integration of effective frequency range, obtain
The seismic imaging result of big gun record.
2. the prestack time migration method based on split-step fast fourier transformation according to claim 1,
It is characterized in that, in step 1, interval velocity model in depth domain is just being drilled with the common big gun collection p obtainingu(t,x,y)
Carry out denoising, these conventional pretreatment of static correction.
3. the prestack time migration method based on split-step fast fourier transformation according to claim 1,
It is characterized in that, the root mean sequare velocity of seed point location in step 2, is picked up by interactive mode,
Smooth the mean-square-root velocity field v obtaining target area through three-dimensional interpolationrms(t, x, y), described root mean sequare velocity
Field is for the step Fourier pre-stack time migration to geological data.
4. the prestack time migration method based on split-step fast fourier transformation according to claim 3,
It is characterized in that, in step 2, using pretreated geological data pu(t, x, y) calculates root-mean-square
Normal-moveout spectrum, by interactive mode, picks up the root mean sequare velocity of seed point location at equal intervals according to 100 meters,
Then the time domain mean-square-root velocity field of the model being spaced apart 10 meters is obtained by interpolation smoothing
vrms(t, x, y), i.e. velocity field needed for pre-stack time migration.
5. the prestack time migration method based on split-step fast fourier transformation according to claim 1,
It is characterized in that, in step 3, based on mean-square-root velocity field vrms(t, x, y), is calculated using ray method
Go out imaging point to the ray propagation time of focal pointWherein, τ is imaging
The time of point, x is the position of imaging point, xsFor the position of focal point, vrmsFor root mean sequare velocity.
6. the prestack time migration method based on split-step fast fourier transformation according to claim 1,
It is characterized in that, in steps of 5, by the mean-square-root velocity field in application time domain, prolonged by single step
Open up and obtain, the mutually transposition of background velocity is directed on continuation time τ, described phase-shift operator expression formula is such as
Under:
Wherein, vrms0(τ) for the background root-mean-square field speed angle value in τ moment, srms0(τ) it is the slow of ambient field
Degree, and srms0(τ)=1/vrms0(τ), w is frequency, kxFor the wave number in x direction, kyFor y direction
Wave number.
7. the prestack time migration method based on split-step fast fourier transformation according to claim 1,
It is characterized in that, in step 6, calculated for step 5 wave field is changed through Fourier inversion
To Frequency-Space Domain, it is calculated by the step Fourier time-displacement operator of time domain on this basis
For the when transposition of Perturbation, apply time-displacement operator, realize the continuation to Perturbation, its expression formula is:
Wherein, δ srms(τ, x, y) is the slowness of Perturbation, so far, completes to the earthquake of geophone station side
The wave field extrapolation in record τ moment at imaging point position.
8. the prestack time migration method based on split-step fast fourier transformation according to claim 1,
It is characterized in that, in step 7, Frequency-Space Domain seismic wave field continuation value that step 6 is obtained,
Move according to firing time image-forming condition implementing phase and effective frequency range is integrated, obtain final
Temporal-spatial field seismic wave field value, its image-forming condition expression formula is:
Wherein, i is the temporal-spatial field seismic wave field after phase shift, and w1 to w2 is seismic wave
Effective band scope.
9. the prestack time migration method based on split-step fast fourier transformation according to claim 1,
It is characterized in that, step 7 also includes: record-shifted for big gun imaging is converted into common imaging gather, closes
And identical geophone offset;All single-shot imaging results are superimposed according to locus, or to common imaging point
Road collection is directly superimposed, and obtains the pre-stack time migration imaging results of target area.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201510394531.8A CN106338766B (en) | 2015-07-07 | 2015-07-07 | Prestack time migration method based on split-step fast fourier transformation |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201510394531.8A CN106338766B (en) | 2015-07-07 | 2015-07-07 | Prestack time migration method based on split-step fast fourier transformation |
Publications (2)
Publication Number | Publication Date |
---|---|
CN106338766A true CN106338766A (en) | 2017-01-18 |
CN106338766B CN106338766B (en) | 2018-09-21 |
Family
ID=57827111
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CN201510394531.8A Active CN106338766B (en) | 2015-07-07 | 2015-07-07 | Prestack time migration method based on split-step fast fourier transformation |
Country Status (1)
Country | Link |
---|---|
CN (1) | CN106338766B (en) |
Cited By (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN110133719A (en) * | 2019-05-23 | 2019-08-16 | 中国石油大学(华东) | Glutenite cascade correlation method based on 90 ° of phase shift data bodies, seed point tracking |
CN112147691A (en) * | 2019-06-28 | 2020-12-29 | 中国石油化工股份有限公司 | Quick coding sequencing-free reference surface correction method and system |
CN112526604A (en) * | 2019-09-17 | 2021-03-19 | 中国石油化工股份有限公司 | Self-adaptive low-frequency compensation method and system based on target layer spectrum analysis |
CN114428324A (en) * | 2022-04-06 | 2022-05-03 | 中国石油大学(华东) | Pre-stack high-angle fast Fourier transform seismic imaging method, system and equipment |
CN115015916A (en) * | 2022-06-22 | 2022-09-06 | 山西华阳集团新能股份有限公司 | Geological radar three-dimensional data offset homing method |
Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2004090573A2 (en) * | 2003-04-07 | 2004-10-21 | Paradigm Geophysical (Luxembourg) S.A.R.L.. | Seimsic imaging by wave migration using a krylov space expansion of the square root exponent operator |
CN1797033A (en) * | 2004-12-29 | 2006-07-05 | 中国石油天然气集团公司 | Method for raising precision of shifted image before superposition by using root mean square velocity |
US20120290213A1 (en) * | 2011-05-13 | 2012-11-15 | Saudi Arabian Oil Company | Frequency-varying filtering of simultaneous source seismic data |
CN102914791A (en) * | 2011-08-05 | 2013-02-06 | 中国石油天然气集团公司 | Kirchhoff prestack time migration method for processing seismic data of undulating surface |
-
2015
- 2015-07-07 CN CN201510394531.8A patent/CN106338766B/en active Active
Patent Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2004090573A2 (en) * | 2003-04-07 | 2004-10-21 | Paradigm Geophysical (Luxembourg) S.A.R.L.. | Seimsic imaging by wave migration using a krylov space expansion of the square root exponent operator |
CN1797033A (en) * | 2004-12-29 | 2006-07-05 | 中国石油天然气集团公司 | Method for raising precision of shifted image before superposition by using root mean square velocity |
US20120290213A1 (en) * | 2011-05-13 | 2012-11-15 | Saudi Arabian Oil Company | Frequency-varying filtering of simultaneous source seismic data |
CN102914791A (en) * | 2011-08-05 | 2013-02-06 | 中国石油天然气集团公司 | Kirchhoff prestack time migration method for processing seismic data of undulating surface |
Non-Patent Citations (1)
Title |
---|
孙涛: "分布傅里叶转换波叠前深度偏移方法研究", 《中国优秀硕士学位论文全文数据库.基础科学辑》 * |
Cited By (10)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN110133719A (en) * | 2019-05-23 | 2019-08-16 | 中国石油大学(华东) | Glutenite cascade correlation method based on 90 ° of phase shift data bodies, seed point tracking |
CN110133719B (en) * | 2019-05-23 | 2020-08-04 | 中国石油大学(华东) | Glutenite period sub-division method based on 90-degree phase shift data volume and seed point tracking |
CN112147691A (en) * | 2019-06-28 | 2020-12-29 | 中国石油化工股份有限公司 | Quick coding sequencing-free reference surface correction method and system |
CN112147691B (en) * | 2019-06-28 | 2024-05-07 | 中国石油化工股份有限公司 | Quick coding ordering-free reference plane correction method and system |
CN112526604A (en) * | 2019-09-17 | 2021-03-19 | 中国石油化工股份有限公司 | Self-adaptive low-frequency compensation method and system based on target layer spectrum analysis |
CN114428324A (en) * | 2022-04-06 | 2022-05-03 | 中国石油大学(华东) | Pre-stack high-angle fast Fourier transform seismic imaging method, system and equipment |
CN114428324B (en) * | 2022-04-06 | 2022-06-28 | 中国石油大学(华东) | Pre-stack high-angle fast Fourier transform seismic imaging method, system and equipment |
US11892578B2 (en) | 2022-04-06 | 2024-02-06 | China University Of Petroleum (East China) | Seismic imaging method, system, and device based on pre-stack high-angle fast Fourier transform |
CN115015916A (en) * | 2022-06-22 | 2022-09-06 | 山西华阳集团新能股份有限公司 | Geological radar three-dimensional data offset homing method |
CN115015916B (en) * | 2022-06-22 | 2024-07-02 | 山西华阳集团新能股份有限公司 | Geological radar three-dimensional data offset homing method |
Also Published As
Publication number | Publication date |
---|---|
CN106338766B (en) | 2018-09-21 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
CN108037526B (en) | Reverse-time migration method based on all-wave wave field VSP/RVSP seismic data | |
CN103091710B (en) | Reverse time migration imaging method and device | |
CN104570124B (en) | A kind of Continuation Imaging method of suitable crosshole seismic wide-angle reflection condition | |
CN106338766A (en) | Pre-stack time migration method based on split-step Fourier algorithm | |
CN102841379B (en) | Method for analyzing pre-stack time migration and speed based on common scatter point channel set | |
CN104730579B (en) | A kind of joint static correcting method of ripple in length and breadth based on calculation of near surface shear velocity inverting | |
CN102841375A (en) | Method for tomography velocity inversion based on angle domain common imaging gathers under complicated condition | |
CN103760603B (en) | The prestack time migration method of converted wave geological data and device | |
CN105589100A (en) | Micro-seismic source location and velocity model simultaneous inversion method | |
CN103995288A (en) | Gauss beam prestack depth migration method and device | |
CN102116869A (en) | High-precision prestack domain least square migration seismic imaging technology | |
CN107656308B (en) | A kind of common scattering point pre-stack time migration imaging method based on time depth scanning | |
CN101598803A (en) | A kind of method that directly obtains stacked section of converted wave | |
CN102866426B (en) | A kind of method utilizing AVO wide-angle road set analysis rock mass hydrocarbon information | |
CN106154319A (en) | A kind of method for separating of imaging road collection | |
CN104237937A (en) | Pre-stack seismic inversion method and system thereof | |
CN102636809A (en) | Method for generating spreading angle domain common image point gathers | |
CN107390270A (en) | A kind of AVA analysis methods based on elastic wave reverse-time migration ADCIGs | |
CN102313903B (en) | Pre-stack time migration method in VTI medium based on wave equation extrapolation operator | |
CN101609167B (en) | Cross-hole seismic wave equation pre-stack depth migration imaging method based on relief surface | |
CN104749623B (en) | A kind of imaging of seismic data processing method | |
CN109116413A (en) | Imaging domain solid chromatographs velocity inversion method | |
CN102798888B (en) | Method for calculating velocity ratio of longitudinal wave to transverse wave by using non-zero wellhead distance data | |
CN107340537A (en) | A kind of method of P-SV converted waves prestack reverse-time depth migration | |
CN106990434B (en) | Ellipse expansion converted wave imaging method and system |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
C06 | Publication | ||
PB01 | Publication | ||
C10 | Entry into substantive examination | ||
SE01 | Entry into force of request for substantive examination | ||
GR01 | Patent grant | ||
GR01 | Patent grant |