Sequential Discontinuities of Feynman Integrals and the Monodromy Group
Sequential Discontinuities of Feynman Integrals and the Monodromy Group Jacob L. Bourjaily1,2, Holmfridur Hannesdottir3, Andrew J. McLeod1, Matthew D. Schwartz3, and Cristian Vergu1 1Niels Bohr International Academy and Discovery Center, Niels Bohr Institute, University of Copenhagen, Blegdamsvej 17, DK-2100, Copenhagen Ø, Denmark 2Institute for Gravitation and the Cosmos, Department of Physics, Pennsylvania State University, University Park, PA 16892, USA 3Department of Physics, Harvard University, Cambridge, MA 02138, USA July 29, 2020 Abstract We generalize the relation between discontinuities of scattering amplitudes and cut diagrams to cover sequential discontinuities (discontinuities of discontinuities) in arbitrary momentum channels. The new relations are derived using time-ordered per- turbation theory, and hold at phase-space points where all cut momentum channels are simultaneously accessible. As part of this analysis, we explain how to compute se- quential discontinuities as monodromies and explore the use of the monodromy group in characterizing the analytic properties of Feynman integrals. We carry out a number of cross-checks of our new formulas in polylogarithmic examples, in some cases to all loop orders. arXiv:2007.13747v1 [hep-th] 27 Jul 2020 Contents 1 Introduction1 2 Cutting rules: a review4 2.1 Cutkosky, 't Hooft and Veltman . .5 2.2 Time-ordered perturbation theory . .7 3 Discontinuities 10 3.1 Covariant approach . 11 3.2 Discontinuities in TOPT . 14 4 Discontinuities as monodromies 17 4.1 Warm-up: the natural logarithm . 17 4.2 The monodromy group . 21 4.3 Monodromies of propagators . 31 5 Sequential discontinuities 33 5.1 Sequential discontinuities in the same channel . 34 5.2 Sequential discontinuities in different channels .
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