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Constraints on current fragments in inclusive lepton scattering

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Lettere al Nuovo Cimento (1971-1985)

An Erratum to this article was published on 01 November 1973

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References

  1. See, for example,S. D. Drell andT. M. Yan:Ann. of Phys.,66, 578 (1971). The current fragments and the target fragments are the two groups of final hadrons associated with the scattered parton and with the unscattered bunch respectively. See ref. (4).S. D. Drell andT. M. Yan:Phys. Rev. Lett.,24, 855 (1970);P. V. Landshoff andJ. C. Polkinghorne:Nucl. Phys.,33 B, 221 (1971).

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  2. J. D. Bjorken:Proceedings of the Tel Aviv Conference on Duality and Symmetry in Hadron Physics, edited byE. Gotsman (Rehovoth, 1971).S. M. Berman, J. D. Bjorken andJ. B. Kogut:Phys. Rev. D,4, 3368 (1971).

  3. The Majumdar-Nachtmann (11). inequality for quark-partons does not use the absence of “hard” interactions between the two groups of fragments in any essential way since it can be derived from lightcone current algebra:C. Gallan, M. Gronau, A. Pais, E. Paschos andS. Treiman:Phys. Rev. D,6, 387 (1972).

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  4. S. D. Drell andT. M. Yan:Phys. Rev. Lett.,24, 855 (1970);P. V. Landshoff andJ. C. Polkinghorne:Nucl. Phys.,33 B, 221 (1971).

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  5. C. H. Llewellyn-Smith andA. Pais:Phys. Rev. Lett.,28, 865, 1356 E (1972).

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  6. In the notation ofDrell andYan (6)\(\ell A_{\dot \iota H}^\mathcal{N} = \int {du_1 F_{\dot \iota }^{\ell \mathcal{N}} } \left( {w,v,u_1 } \right).\). N.B.\(w \equiv \omega ^{ - 1} \) and\(v \equiv \omega _L^{ - 1} \).

  7. For the definition of this function, see eq. (9). of Drell and Yan’s paper (4).S. D. Drell andT. M. Yan:Phys. Rev. Lett.,24, 855 (1970);P. V. Landshoff andJ. C. Polkinghorne:Nucl. Phys.,33 B, 221 (1971).

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  8. O. Nachtmann:Nucl. Phys.,38 B, 397 (1972). See alsoP. Roy:Theoretical ideas on lepton-hadron processes.—I:Partons, Tata Institute of Fundamental Research Lectures.

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  9. H. Lipkin andE. Paschos:Phys. Rev. Lett.,29, 525 (1972).

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  10. J. Ellis:Phys. Lett.,35 B, 537 (1971);J. D. Stack:Phys. Rev. Lett.,28, 57 (1972);O. Nachtmann:Phys. Rev. D,6, 1718 (1972).

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  11. D. P. Majumdar:Phys. Rev. D,3, 2869 (1971);O. Nachhtmann: ref. (8).Nucl. Phys.,38 B, 397 (1972).

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  12. M. Gronau, P. Ravndal andY. Zarmi: California Institute of Technology Report No. 68-367, to be published.

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  1. Tata Institute of Fundamental Research, Bombay

    P. Roy

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  1. P. Roy
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An erratum to this article is available at http://dx.doi.org/10.1007/BF02891931.

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Roy, P. Constraints on current fragments in inclusive lepton scattering. Lett. Nuovo Cimento 7, 175–179 (1973). https://doi.org/10.1007/BF02746353

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