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Froissart bound for inelastic cross sections
We prove that while the total cross{}-section is bounded by $(\pi/m_\pi^2) \ln^2 s$, where $s$ is the square of the c.m. energy and $m_\pi$ the mass of the pion, the total inelastic cross{}-section is bounded by $(1/4)(\pi/m_\pi^2) \ln^2 s$, which is 4 times smaller. We discuss the implications of t...
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| Lenguaje: | eng |
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2009
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| Acceso en línea: | https://dx.doi.org/10.1103/PhysRevD.80.065013 http://cds.cern.ch/record/1174013 |