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t° ] F |2 a Jv. From mere dimensional considerations it can easily be seen th at terms of W proportional to l/rn give a contribution to the crosssection which asymptotically depends on v like vn~^. Thus our asymptotic formula (42) ( 0~l/^v ) is due to the 1/r3 terms in the proton ne interaction.] References Bethe and Bacher 1936 Rev. Mod. Phys. 8, 82.doi:10.1098/rspa.1940.0008 fatcat:qcx2hxiwqbgbbg2vocczawjwry