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Froissart bound

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In particle physics the Froissart bound, or Froissart limit, is a generic constraint that the total scattering cross section of two colliding high-energy particles cannot increase faster than c×ln2(s), with c a normalization constant and s the square of the center-of-mass energy (s is one of the three Mandelstam variables).[1]

Further reading

The Froissart bound on scholarpedia, by M. Froissart

References

  1. ^ Froissart, Marcel (1961). Asymptotic Behavior and Subtractions in the Mandelstam Representation. Physical Review 123 (3): 1053-1057.


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