Froissart bound
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[]
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