Publisher
Springer Science and Business Media LLC
Subject
General Physics and Astronomy
Reference12 articles.
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).
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).
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).
5. C. H. Llewellyn-Smith andA. Pais:Phys. Rev. Lett.,28, 865, 1356 E (1972).
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