Abstract
A convergent integral representation for the massive Feynman amplitude in complex dimension D is defined away from ReD equal to some rationals. The Feynman integrand is modified according to the technique of Zimmermann’s forests but each subgraph is subtracted at zero external momenta and zero internal masses; the order of the Taylor subtractions depends upon ReD. The so defined regularized Feynman amplitude is a meromorphic function of D with multiple poles at some rationals, which satisfies field equations and Ward identities. These amplitudes may be used in the construction of a bare Lagrangian field theory.
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.
