Abstract
Let F be a finite field and G=GL(6,F). In this paper, we explicitly describe the structure of the twisted Jacquet module πN,ψA where A is a rank 2 matrix and π is an irreducible cuspidal representation of G.
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Disclaimer: 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.