1966
DOI: 10.1002/prop.19660140117
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Dispersion Analysis of Elastic Scattering of High Energy Particles

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1968
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Cited by 8 publications
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“…In the calculations we have taken a N (t) = a N (Q) where the a p (0) and a n (0) have been obtained from Barashenkov. 6 The total pion-nucleon cross sections were measured by Citron et al, 7 and the diffraction slopes were fitted by Lasinski, Levi Setti, and Predazzi. 8 The Hamada-Johnston deuteron wave function was used to determine the form factors.…”
Section: Mq) = Jf[i+ A^i^l^y^xpiujvt) N = Narp T=-q\mentioning
confidence: 99%
“…In the calculations we have taken a N (t) = a N (Q) where the a p (0) and a n (0) have been obtained from Barashenkov. 6 The total pion-nucleon cross sections were measured by Citron et al, 7 and the diffraction slopes were fitted by Lasinski, Levi Setti, and Predazzi. 8 The Hamada-Johnston deuteron wave function was used to determine the form factors.…”
Section: Mq) = Jf[i+ A^i^l^y^xpiujvt) N = Narp T=-q\mentioning
confidence: 99%