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Quantum field theory and the Bieberbach conjecture
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An intriguing correspondence between ingredients in geometric
function theory related to the famous Bieberbach conjecture (de Branges’
theorem) and the non-perturbative crossing symmetric representation of
2-2 scattering amplitudes of identical scalars is pointed out. Using the
dispersion relation and unitarity, we are able to derive several
inequalities, analogous to those which arise in the discussions of the
Bieberbach conjecture. We derive new and strong bounds on the ratio of
certain Wilson coefficients and demonstrate that these are obeyed in
one-loop \phi^4ϕ4
theory, tree level string theory as well as in the S-matrix bootstrap.
Further, we find two sided bounds on the magnitude of the scattering
amplitude, which are shown to be respected in all the contexts mentioned
above. Translated to the usual Mandelstam variables, for large
|s||s|,
fixed tt,
the upper bound reads |\mathcal{M}(s,t)|\lesssim |s^2||ℳ(s,t)|≲|s2|.
We discuss how Szeg"{o}’s theorem corresponds to a check of
univalence in an EFT expansion, while how the Grunsky inequalities
translate into nontrivial, nonlinear inequalities on the Wilson
coefficients.
Title: Quantum field theory and the Bieberbach conjecture
Description:
An intriguing correspondence between ingredients in geometric
function theory related to the famous Bieberbach conjecture (de Branges’
theorem) and the non-perturbative crossing symmetric representation of
2-2 scattering amplitudes of identical scalars is pointed out.
Using the
dispersion relation and unitarity, we are able to derive several
inequalities, analogous to those which arise in the discussions of the
Bieberbach conjecture.
We derive new and strong bounds on the ratio of
certain Wilson coefficients and demonstrate that these are obeyed in
one-loop \phi^4ϕ4
theory, tree level string theory as well as in the S-matrix bootstrap.
Further, we find two sided bounds on the magnitude of the scattering
amplitude, which are shown to be respected in all the contexts mentioned
above.
Translated to the usual Mandelstam variables, for large
|s||s|,
fixed tt,
the upper bound reads |\mathcal{M}(s,t)|\lesssim |s^2||ℳ(s,t)|≲|s2|.
We discuss how Szeg"{o}’s theorem corresponds to a check of
univalence in an EFT expansion, while how the Grunsky inequalities
translate into nontrivial, nonlinear inequalities on the Wilson
coefficients.
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