Tables

Abstract

Each Feynman integral presented here can be evaluated straightforwardly by use of alpha or Feynman parameters. Results are presented for the ‘Euclidean’ dependence, −k ², of the denominators, which is more natural when the powers of propagators are general complex numbers. As usual, −k ² is understood in the sense of −k ² − i0, etc. Moreover, denominators with a linear dependence on k are also understood in this sense, e.g. 2p ⋅k 2p ⋅k−i0, although sometimes this i0 dependence is explicitly indicated to avoid misunderstanding.