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The axial vector form factor of the nucleon and the quark-parton model

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Lettere al Nuovo Cimento (1971-1985)

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Footnotes

  1. K. Kitani andH. Yoshii:Lett. Nuovo Cimento,4, 431 (1970).

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  2. S. D. Drell andT. M. Yan:Phys. Rev. Lett.,24, 181 (1970).

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  3. E. D. Bloom andF. J. Gilman:Phys. Rev. Lett.,25, 1140 (1970).

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  4. Y. Nambu andM. Yoshimura:Phys. Rev. Lett.,24, 25 (1970). See alsoE. Amaldi, B. Borgia, P. Pistilli, M. Balla, G. V. Di Giorgio, A. Giazotto, S. Serbassi andG. Stoppini:Nuovo Cimento,65 A, 377 (1970).

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  5. On this point seeK. Kitani, Y. Nagatsuka andH. Yoshii:High-energy elastic hadron-hadron scattering and electromagnetic structure of the hadron, Tokyo Institute of Technology preprint.

  6. For electron-nucleon scattering the B-G conjecture andG 2 E /Q 2G 2 M →0 asQ 2→∞ lead us to νW 2=2MxW 1 (orσ S /σ T = 0) nearx=1 (12), which implies within the parton model that partons with spin 1/2 dominate even atx=1, contrary to the D.L.Y. model:S. D. Drell, D. J. Levy andT. M. Yan:Phys. Rev. D,1, 1035 (1970).

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  7. F. J. Gilman:Recent developments in inelastic electron-nucleon scattering, SLAC-PUB-842.

  8. S. Weinberg:Phys. Rev. Lett.,18, 507 (1967).

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  1. Department of Physics, Tokyo Institute of Technology, Tokyo

    K. Kitani, R. Tanabe & H. Yoshii

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  1. K. Kitani
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  2. R. Tanabe
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  3. H. Yoshii
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Kitani, K., Tanabe, R. & Yoshii, H. The axial vector form factor of the nucleon and the quark-parton model. Lett. Nuovo Cimento 2, 789–793 (1971). https://doi.org/10.1007/BF02789644

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  • DOI: https://doi.org/10.1007/BF02789644

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