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- W2061151103 abstract "It is shown that at sufficiently large $N_c$ for incident momenta which are much larger than the QCD, the total nucleon-nucleon cross section is independent of incident momentum and given by $sigma^{rm total}=2 pi log^2(N_c) / (m^2_{pi})$. This result is valid in the extreme large $N_c$ regime of $log(N_c) gg 1$ and has corrections of relative order $log (log(N_c))/log(N_c)$. A possible connection of this result to the Froissart-Martin bound is discussed." @default.
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- W2061151103 date "2012-06-26" @default.
- W2061151103 modified "2023-09-27" @default.
- W2061151103 title "Total Nucleon-Nucleon Cross Section at LargeNc" @default.
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- W2061151103 doi "https://doi.org/10.1103/physrevlett.108.262301" @default.
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