Abstract
The construction of a 3-D Kirchhoff dip moveout (DMO) operator for the constant‐velocity case is remarkably simple in concept. First, generate the 2-D DMO operator between the source and receiver and then place it in the desired output 3-D volume along the trajectory between the source and receiver. Most of the literature concerning the design of such operators addresses the first step in the process, i.e., generation of the 2-D DMO operator. This paper treats the second part: sampling the 2-D DMO operator into the 3-D volume.
Sign-in/Register to access full text options 
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Schedule a callDisclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.
