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Mandelstam analyticity: single-function description across the entire Mandelstam plane

Establish rigorously that there exists a single analytic function T(s,t) that simultaneously describes a given 2→2 scattering process and all of its crossed channels throughout the entire Mandelstam plane, including all three physical regions, under the assumptions of analyticity and crossing symmetry.

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Background

In discussing 2→2 scattering with Mandelstam variables s, t, and u, the chapter emphasizes that analyticity and crossing symmetry motivate viewing the amplitude as a single analytic function T(s,t) defined over the full Mandelstam plane, covering all physical regions and crossed channels. This global analyticity assumption is historically associated with the Mandelstam analyticity program in S-matrix theory.

While the text notes that this viewpoint can be justified from non-relativistic scattering theory, axiomatic quantum field theory, and analyses of perturbative Feynman diagrams, it explicitly refers to the statement as a conjecture rather than a theorem. A rigorous, fully general proof remains a central conceptual challenge in the analytic S-matrix framework.

References

Analyticity and crossing symmetry dictate that there is a single analytic function T(s,t) that describes the scattering reaction and all its crossed channels in the whole Mandelstam plane, including all three physical regions. This conjecture can be justified from knowledge on non-relativistic quantum mechanical scattering, axiomatic quantum field theory, and the study of (perturbative) Feynman diagrams.

Dispersion relations: foundations (2510.01962 - Kubis, 2 Oct 2025) in Section "Some remarks on dispersion relations for scattering processes" (opening paragraph)