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For the possibility of the large OZI violation in the axial vector channel and its relation to the nucleon spin problem, see G. Altarelli and G. Ridolfi, QCD 94, Proceedings of the International Conference, Montpellier, France, 1994, edited by S. Narison, [Nucl. Phys. B (Proc. Suppl.) 39B, C, 106 (1995)].NPBSE7
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The current status of the lattice simulation in the flavor singlet channel is summarized in M. Okawa, in Lattice ’95, Proceedings of the International Symposium, Melbourne, Australia, edited by T. O. Kieu [Nucl. Phys. B (Proc. Suppl.) 47, 160 (1996)].NPBSE7
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A preliminary report of the this study was presented at the Australia-Japan workshop on Quarks, Hadrons and Nuclei, Adelaide, Australia, 1995 (unpublished) and at the RIKEN Symposium on Spin Structure of the Nucleon, RIKEN, Japan, 1995; University of Tsukuba Report No. UTHEP-337, hep-lat/9606006 (unpublished)
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A preliminary report of the this study was presented at the Australia-Japan workshop on Quarks, Hadrons and Nuclei, Adelaide, Australia, 1995 (unpublished) and at the RIKEN Symposium on Spin Structure of the Nucleon, RIKEN, Japan, 1995; University of Tsukuba Report No. UTHEP-337, hep-lat/9606006 (unpublished).
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For lattice QCD simulations of the moments of the structure functions (Formula presented) and (Formula presented), see the recent review by M. Göckeler et al., in Lattice ’96, Proceedings of the International Symposium, St. Louis, Missouri, edited by C. Bernard et al. [Nucl. Phys. B (Proc. Suppl.) 53, 81 (1997)], hep-lat/9608046.NPBSE7
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Here we use Minkowski notation with the Bjorken-Drell convention
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Here we use Minkowski notation with the Bjorken-Drell convention.
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G. P. Lepage, in Lattice ’95 [4], p. 3.
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