Systems and methods for pre-correlation noise attentuation using random sweeps in seismic data processing
US-2015241586-A1 · Aug 27, 2015 · US
US9804283B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-9804283-B2 |
| Application number | US-201414897002-A |
| Country | US |
| Kind code | B2 |
| Filing date | Jun 26, 2014 |
| Priority date | Jun 28, 2013 |
| Publication date | Oct 31, 2017 |
| Grant date | Oct 31, 2017 |
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Methods and systems for separating seismic data acquired using a plurality of substantially simultaneously fired sources are described. The sources use sweep sequences having low cross correlation levels to generate seismic waves, and their source signatures are determined. Using the source signatures, the wave fields associated with each of the sources are extracted from the seismic data by, for example, performing a time domain deconvolution.
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What is claimed is: 1. A method for separating seismic data, said method comprising: firing two or more sources in a time overlapping manner using sweep sequences that have low-level cross-correlations, wherein one of the at least two or more sources generates seismic waves using a first sweep sequence and another of the at least two or more sources generates seismic waves using a second sweep sequence, and wherein the low-level cross-correlation is defined as a ratio between (i) a maximum of an auto-correlation of one of the first sweep sequence and the second sweep sequence, and (ii) a mean level of cross-correlation between the first sweep sequence and the second sweep sequence, acquiring seismic data R associated with the firing of the two or more sources; recording a source signature S k for each of the two or more sources; and extracting, by applying a convolution model, a wave field E k associated with each of the two or more sources using the seismic data R and the source signatures S k , wherein the convolution model considers that the seismic data R is a sum of convolutions of corresponding source signatures S k and wave fields E k , a matrix S associated with the source signatures S k is a convolution operator, the wave fields E k are obtained by using the seismic data R and a matrix S T S, which is a product of (i) a transpose S T of the matrix S and (ii) the matrix S, matrix S T S has non-diagonal terms that are cross-correlations of the source signatures S k , and matrix S T S has diagonal terms that are autocorrelations of the source signatures S k . 2. The method of claim 1 , wherein the second sweep sequence is different than the first sweep sequence. 3. The method of claim 1 , wherein a low-level cross-correlation value is less than a predetermined threshold value. 4. The method of claim 1 , wherein the sweep sequences with low-level cross correlations are one of: slip sweep sequences, sine waves having synchronized phase rotations with or without listening time, sine waves having unsynchronized phase rotations and random sequences. 5. The method of claim 1 , wherein the source signatures are one of: near field measurements of outputs of each of the two or more sources, measurements of the two or more sources' actuator motion or pressure, or time-stamped sweep sequences. 6. The method of claim 5 , wherein the source signatures are generated using a weighted sum of outputs of accelerometers located on a vibrator plate and a vibrator mass of each of the at least two sources. 7. The method of claim 1 , wherein the step of extracting further comprises: solving the convolution model from a continuous recording of seismic data. 8. The method of claim 7 , wherein the step of extracting further comprises: performing a time domain deconvolution process using the acquired seismic data and the source signatures. 9. The method of claim 7 , wherein the step of extracting further comprises: applying a conjugate-gradient algorithm to the seismic data. 10. The method of claim 9 , wherein the conjugate gradient algorithm is performed in two or more iterations. 11. A system for processing seismic data, said system comprising: at least one processor which is configured to receive (1) recorded seismic data R associated with the firing of two or more sources in a time overlapping manner using sweep sequences that have low-level cross-correlations and (2) a source signature S k for each of the two or more sources, wherein one of the at least two or more sources generates seismic waves using a first sweep sequence and another of the at least two or more sources generates seismic waves using a second sweep sequence, and wherein the low-level cross-correlation is defined as a ratio between (i) a maximum of an auto-correlation of one of the first sweep sequence and the second sweep sequence, and (ii) a mean level of cross-correlation between the first sweep sequence and the second sweep sequence; and wherein the at least one processor is further configured to extract, by applying a convolution model, a wave field E k associated with each of the two or more sources using the seismic data R and the source signatures S k , wherein the convolution model considers that the seismic data R is a sum of convolutions of corresponding source signatures S k and wave fields E k , a matrix S associated with the source signatures S k is a convolution operator, the wave fields E k are obtained by using the seismic data R and a matrix S T S, which is a product of (i) a transpose S T of the matrix S and (ii) the matrix S, matrix S T S has non-diagonal terms that are cross-correlations of the source signatures S k , and matrix S T S has diagonal terms that are autocorrelations of the source signatures S k . 12. The system of claim 11 , wherein the second sweep sequence is different than the first sweep sequence. 13. The system of claim 12 , wherein a low-level cross-correlation value is less than a predetermined threshold value. 14. The system of claim 11 , wherein the sweep sequences with low-level cross correlations are one of: slip sweep sequences, sine waves having synchronized phase rotations with or without listening time, sine waves having unsynchronized phase rotations and random sequences. 15. The system of claim 11 , wherein the source signatures are one of: near field measurements of outputs of each of the two or more sources, measurements of the two or more sources' actuator motion or pressure, or the sweep sequences. 16. The system of claim 15 , wherein the source signatures are generated using a weighted sum of outputs of accelerometers located on a vibrator plate and a vibrator mass of each of the at least two sources. 17. The system of claim 11 , wherein the at least one processor is further configured to extract the wave fields by solving the convolution model from a continuous recording of seismic data. 18. The system of claim 17 , wherein the at least one processor is configured to extract the wave fields by performing a time domain deconvolution process using the acquired seismic data and the source signatures. 19. The system of claim 17 , wherein the at least one processor is extract the wave fields by applying a conjugate-gradient algorithm to the seismic data. 20. A non-transitory computer-readable medium, having program instructions stored thereon which, when executed by a suitably programmed computing device, performs the steps of: firing two or more sources in a time overlapping manner using sweep sequences that have low-level cross-correlations, wherein one of the at least two or more sources generates seismic waves using a first sweep sequence and another of the at least two or more sources generates seismic waves using a second sweep sequence, and wherein the low-level cross-correlation is defined as a ratio between (i) a maximum of an auto-correlation of one of the first sweep sequence and the second sweep sequence, and (ii) a mean level of cross-correlation between the first sweep sequence and the second sweep sequence, acquiring seismic data R associated with the firing of the two or more sources; recording a source signature S k for each of the two or more sources; and extracting, by applying a convolution model, a wave field E k associated with each of the two or more sources using the seismic data R and the source signatures S k , wherein the convolution model considers that the seismic data R is a sum of convolutions of corresponding source signatures S k and wave fields
with exploration systems emitting special signals, e.g. frequency swept signals, pulse sequences or slip sweep arrangements · CPC title
Correlating received seismic signals with the emitted source signal · CPC title
Corrections or adjustments related to wave propagation · CPC title
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