In a case study from the Austrian Alps, the capability of Common-Reflection-Surface processing (CRS) for comprehensive fault imaging and analysis is demonstrated. CRS processing is used to generally improve the signal-to-noise ratio and to regularize the dataset in different domains. We show an offset-azimuth regularization to generate well populated gathers in six different azimuth classes. Each azimuth class is separately Kirchhoff-migrated to image faults according to their orientation. For a Reverse Time Migration (RTM) a dataset is shot-receiver regularized. The CRS signal enhancement generally improves the resolution of the subsurface structures, while the regularization minimizes operator noise.

Introduction

Seismic resolution is often limited by a low signal-to-noise ratio, and by numerous data gaps and coverage irregularities. Various processing strategies to reduce these problems are provided by CRS processing based on the Common-Reflection-Surface method. CRS attributes calculated from the seismic wavefield describe the reflection events in detail, and allow to improve the seismic signal over random noise. In the vicinity of existing data, the detailed CRS event description may also be used to reconstruct missing traces. This approach cannot only be applied to fill data gaps, but also to regularize data in different domains.

In a case history from the Alpine Mountains in Austria, we test the advantages of CRS offset-azimuth regularization, and of CRS shot-receiver regularization for different imaging and interpretation aspects. The offset-azimuth regularization is used to generate well populated gathers in different azimuth classes that are migrated separately. The major faults of the subsurface are resolved in all azimuth classes, whereas small, more subtle features are imaged in individual classes with more profound orthogonal illumination.

Offset-azimuth regularization optimizes subsurface coverage which customizes the data for Kirchhoff type migrations, but does not preserve a surface acquisition geometry. Shot-receiver regularization, on the contrary, optimizes the surface coverage by a regular acquisition geometry. This provides a regular distribution of input data for migration in the shot domain, but does not fully normalize the subsurface fold. However, Reverse Time Migration (RTM) as a sophisticated two-way wave equation in shot domain, should benefit from a regular surface coverage.

Method

A sophisticated strategy of time domain stacking of seismic data beyond NMO stacking was first presented by Gelchinsky (1988), taking into account a complex lateral inhomogeneity of the subsurface. Based on these ideas, the common reflection surface (CRS) stack was then designed by Hubral et al. 1999, Mann et al. 1999, and Jäger et al. 2001. CRS stacking is a robust and powerful methodology for seismic data enhancement that has been successfully adapted to exploration seismic during recent years, e.g. Eisenberg-Klein et al. 2008, Trappe et al. 2011, and Pruessmann et al. 2012.

The principle of CRS stacking is summarized in Fig. 1. The seismic data is parameterized according to dipping and curved reflector elements in the subsurface that generate the acquired reflected wavefield. For each event, CRS wavefield attributes related to a point source and to an exploding reflector segment are derived directly from the seismic data. These CRS attributes describe the travel time of a reflection event across several CMP locations. Due to this extended validity, these CRS traveltime surfaces hardly coincide with random noise. As a result, the seismic image is cleaned from random noise, showing an improved resolution and event continuity.

Fig. 01
Figure 1. The CRS attributes (α, RNIP, RN) that define a CRS stacking surface for a seismic reflection event are visualized by two related wavefields that may be generated first by a point source at the normal incidence point (a), and second by an exploding reflector segment (b). At the central stacking location XO, the corresponding wavefronts are observed at the emergence angle α with curvatures RNIP or RN, respectively (after Jäger et al. 2001).

The excellent fit of the CRS stacking surface to a reflection event is illustrated by comparing conventional DMO stacking (c) to CRS stacking (d). For the anticlinal model in the lower part of the graphs, the common-offset travel time functions (blue) are displayed above for CMP location x and half-offset h. The DMO stacking surface (green) collects the reflection event (blue) only in a small tangential area along the solid green line (c), whereas CRS stacking (green) well follows the event in a large area (d, after Hubral et al. 1999).

With the CRS technique it is possible to reconstruct missing traces in a seismic data set by mapping seismic event data along the CRS traveltime surfaces. This interpolation can be used in any type of data regularization, or specifically in order to fill certain acquisition gaps. Unlike other interpolation algorithms (e.g. 5-D interpolation) CRS processing can handle data from complex geology and steep-dip reflectors (Fig. 2). The selected type of regularization depends on the intended processing and imaging sequence. For Kirchhoff prestack migration a regularization in CMP-offset domain is the preferred choice, whereas for depth migration in the shot domain by RTM a shot-receiver regularization is adequate.

Fig. 02
Figure 2. Stacks of raw data, 5-D interpolation, and CRS processing for a 3-D seismic data set onshore, showing a vertical section (top row), and a time slice (bottom row). Note the improved signal-to-noise ratio throughout the vertical CRS section. The CRS processing reconstructs seismic data only in a certain vicinity of reliable information, thus leaving a gap in the time slice (bottom right).

Alpine data set

The data set processed in this case history was acquired in the transition zone between the Northern Calcareous Alps and the Molasse Foreland Basin, Austria. The Molasse Foreland Basin covers a vast area north of the Alps, and deepens southwards towards the Alps. The Molasse sediments are divided in three sections: Tertiary Molasse, Imbricated Molasse, and Subalpine Molasse. The Imbricated Molasse is associated with the nappe tectonics of the Alps. These nappes were formed by the north-south oriented stress field, and thus are divided by mainly east-west striking faults.

Table 1. Acquisition parameters for the 3-D seismic data set, Northern Calcareous Alps
source line spacing: 500 m
source point spacing: 50 m
receiver line spacing: 200 m
receiver point spacing: 50 m
receiver points per patch line: 120
symmetric split spread
receiver lines per spread: 16
number of channels per spread: 1920
nominal coverage: 48 fold

The seismic data was acquired in several 3-D surveys (from 1984 to 2004). The data examples shown here are taken from the latest data set, with parameters being summarized in table 1. Receiver lines are mainly oriented north-southwards with orthogonal shot lines to best image the east-west striking faults.

CRS processing and Kirchhoff migration

The initial processing approach comprised a general appraisal of the image improvement to be expected from the CRS method. A traditional CRS offset regularization significantly enhanced the signalto- noise ratio and the continuity of reflectors in the complicated thrust geology. In Fig. 3, the resolution of thrust planes and anticlines in time migration is superior by prior CRS data preconditioning, than by conventional time processing.

Fig. 03
Figure 3. Prestack time migration of a third party contractor with standard time processing (left), versus post-stack time migration with CRS processing.

Departing from this initial CRS performance, the CRS technique was used to regularize the data in offset and azimuth domain, using equidistant azimuth sectors. Due to shot-receiver reciprocity the valid azimuth variation is reduced to the range of 0° – 180° which was covered by six azimuth classes of 30°. The decomposition of the original data into these azimuth classes obviously resulted in very low fold levels as an individual class comprises 5 to 10 traces on average (Fig. 4).

CRS regularization then largely reconstructed the missing traces from the available wavefield. In the azimuth sectors, the fold level was increased to a level between 20 and 40 (Fig. 4). However, not all azimuth sectors were completely filled: In the sectors bordering to 90° (east-west direction) only near-offset traces were available. This was due to the north-south layout of the acquisition.

Fig. 04
Figure 4. (Top) An original CMP gather is decomposed into six azimuth classes that are offset-sorted internally; fold maps of these azimuth classes show the example bin as a black dot, and generally low fold levels up to 10. (Bottom) After CRS offset-azimuth regularization, the same CMP bin is more densely populated at all six azimuth classes, which is also reflected by the fold maps.

The well filled CRS azimuth gathers were then migrated separately using a Kirchhoff algorithm. Within each azimuth class different fault details and geologic features are visible (Fig. 5), which implicates a more detailed interpretation of fault and fracture orientation. Although the main fracture orientation is east-west, the azimuth classes near 90° emphasize some additional faults, which run north-south. In Fig. 5, a northern and a southern fault are interpreted in the zoomed sections of the single azimuth migrations. While the northern fault is visible on all azimuth classes, the southern fault vanishes in the two classes near 90°. This fault is either a small north-south trending feature, that only appears when illuminated at a right angle. It can also be a phantom fault, induced on the seismic data by the complicated geology overlying this region.

Fig. 05
Figure 5. Kirchhoff prestack time migration after CRS offset-azimuth regularization. The center image shows the full-azimuth migration of an arbitrary inline, oriented north-south. The zooms are extracted from the separately migrated azimuth classes, with azimuth ranges indicated next to the individual images. The thin black lines indicate a northern and a southern fault. Notice that the southern fault is not visible on all azimuth classes.

Reverse Time Migration

Reverse Time Migration (RTM) is an advanced depth migration method based on two-way wave equation modeling of source and receiver wavefields that are combined by an imaging condition. The imaging condition, commonly a wavefield correlation, transforms the modeled wavefields to the final depth image.

RTM is considered to be the most adequate migration algorithm for complex tectonic settings, which has been demonstrated in a wide range of applications. However, most of the case studies discussed in literature are marine data examples. One of the reasons for the absence of land data may be the reduced fold and low signal-to-noise ratio, often combined with irregular geometry. In this case study, the combination of CRS and RTM was tested on a complex land dataset as promising approach to overcome these disadvantages.

The RTM modeling used a pseudo-spectral code based on fast Fourier transformations (FFT) to solve the spacial derivatives of the seismic wavefield. This approach is more accurate than FD operators due to the large operator size: The FFT code processes the complete extension of the seismic model concurrently, while the FD approach only uses the neighboring samples.

Fig. 6 demonstrates the impact of CRS processing in combination with prestack depth migration using different algorithms. The Fig. 6a) and 6b) illustrate the use of conventional NMO gathers versus CRS offset-regularized gathers in Kirchhoff depth migration. Especially in the upper part of the central fault zone, the CRS processing increases the event continuity and resolution.

Fig. 06
Figure 6. Inline sections of prestack depth migration in a 3-D land dataset. a) Kirchhoff migration of NMO gathers. b) Kirchhoff migration of CRS offset-regularized gathers. c) RTM of CRS shot gathers.

In order to reconstruct the deeper part of the fault zone from wavefield contributions with increasing complexity, we move from ray-based migration to wave-equation migration. Figs. 6b) and c) compare ray-based Kirchhoff depth migration of CRS offset-regularized gathers to RTM of CRS shot gathers. The CRS-based RTM image improves the depth resolution throughout the section, clarifying the main structural units and faults from shallow details down to large depths. Although the frequency content is lower than in Kirchhoff migration, the structural information is significantly improved in the RTM.

Conclusion

This case study applies a CRS processing as a well established technology to improve the continuity and overall signal-to-noise ratio of seismic reflection data. Due to its detailed parameterization of the entire wavefield, the CRS methodology additionally provides a flexible regularization and data reconstruction at acquisition gaps which is superior to a 5-D interpolation result. For different migration algorithms, different types of CRS regularization are demonstrated to solve the imaging and interpretation tasks.

A CRS regularization in the offset-azimuth domain is used to produce well populated azimuth classes that are subsequently input to individual Kirchhoff migrations. The major faults of the subsurface are resolved in all azimuth classes, whereas small, more subtle features are imaged in individual classes with more profound orthogonal illumination. This azimuthal regularization and imaging is thus providing both, more details of the subsurface geology, and additional confirmation on the orientation of small features.

A CRS regularization in the shot-receiver domain provides a uniform areal shot coverage as input to Reverse Time Migration (RTM). The regular CRS shot gathers minimize migration footprints in RTM imaging, and the enhanced signal-to-noise ratio of the CRS processing improves the seismic events in general. It thus provides a strong increase in resolution of the complex subsurface structures, and compensates for the typical irregularity issues of these low-fold seismic land data.

End

     

About the Author(s)

Henning Trappe is Managing Director and founder of TEEC in Isernhagen, Germany. He studied Physics and Geophsics at Kiel University in Germany. After finishing his Ph.D. thesis he joined BEB Erdöl Erdgas GmbH (at that time an Exxon and Shell subsidiary) before he founded TEEC in 1992. His professional experience covers concession & prospect evaluation, reservoir geophysics, geophysical data interpretation and processing.

Eliakim Schuenemann studied and received his Diploma in Geophysics at the University of Karlsruhe, Germany in 2007. After that he joined for a short time the tectonic stress group at the same university. From 2008 to 2009 he worked in the tunneling business on a seismic prediction system. Since 2009 he works as an R&D geophysicist for TEEC GmbH.

Juergen Pruessmann received a Ph.D. in geophysics in 1994 from the University of Hamburg, Germany. Since then he has been working in seismic processing and development with several seismic contractors in Germany. In 2001, he joined TEEC where he presently is the head of research and development. His research interests are focused on seismic methods including imaging and model building, neural network and coherency methods, AVO and reservoir characterization.

Sonja Suckro started at the TEEC GmbH in 2013 as processing geophysicist. She has a diploma in Geophysics from the University of Muenster, Germany, where she focused on ground penetrating radar surveys. In 2008, she proceeded to the Alfred Wegener Institute for Polar and Marine Research, Bremerhaven, Germany, for marine seismic studies in the Baffin Bay area. During this time she completed her Ph.D. at the University of Bremen, Germany. Sonja Suckro is a member of the EAGE, DGG, DGP.

Hans-Gert Linzer has a master´s degree and Ph.D. in Geology from the University of Karlsruhe (KIT). His postdoctoral research experience in complex deformed fold thrust belts included work at University of Tuebingen, Rice University and Amoco (Houston, Texas). He left 1998 academia to work as a structural and exploration geologist with RAG, Vienna in the foreland basin and fold belt of the Alps. Gert is member of AAPG and ÖGEW.

Martin Schachinger has been Supervisor, Seismic Acquisistion and Processing, at Rohöl-Aufsuchungs AG (RAG) in Vienna, Austria, since 2005. He began his career in 1989 with Prakla-Seismos as processing geophysicist at the Vienna Data Centre, where he subsequently worked as data center manager. He also served as supervisor standard data processing at the Geco- Prakla Hannover Data Center in Germany. He joined RAG in 2000 as a staff geophysicist involved in seismic acquisition and processing. He earned a Ph.D. degree in geophysics at University of Vienna.

References

Eisenberg-Klein, G., Pruessmann, J., Gierse, G., and Trappe, H. (2008). Noise Reduction in 2D and 3D seismic imaging by the CRS method. The Leading Edge, 27(2), 258 – 265.

Gelchinsky, B. (1988), The common reflecting element (CRE) method (non-uniform asymmetric multifold system). Exploration Geophysics, 19(1/2), 71-75.

Hubral, P., Hoecht, G., and Jaeger, R. (1999). Seismic illumination. Leading Edge, 18(11), 1268 – 1271.

Jaeger, R., Mann, J., Hoecht, G., and Hubral, P. (2001). Common-reflection-surface stack: Image and attributes. Geophysics, 66(1), 97 – 109.

Mann, J., Jaeger, R., Mueller, T., Hoecht, G., and Hubral, P. (1999). Commonreflection- surface stack – a real data example. Journal of Applied Geophysics, 42 (3-4), 301-318.

Pruessmann, J., Gierse, G., Trappe, H. (2012). Look closer at your reservoir. Oilfield Technology, May 2012, 28 – 32.

Trappe, H., Eisenberg-Klein, G., Pruessmann, J., 2011. Sharpened Vision. Oilfield Technology, June 2011.

Appendices

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