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  • Collaboration, CCFR; Tamminga, B H; Adams, T; Alton, A; Arroyo, C G; Avvakumov, S; de Barbaro, L; de Barbaro, P; Bazarko, A O; Bernstein, R H; Bodek, A; Bolton, T; Brau, J; Buchholz, D; Budd, H; Bugel, L; Conrad, J; Drucker, R B; maggio, J A; Frey, R; Goldman, J; Goncharov, M; Harris, D A; Johnson, R A; Kim, J H; King, B J; Kinnel, T; Koutsoliotas, S; Lamm, M J; Marsh, W; Mason, D; McFarland, K S; McNulty, C; Mishra, S R; Naples, D; Nienaber, P; Romosan, A; Sakumoto, W K; Schellman, H; Sciulli, F J; Seligman, W G; Shaevitz, M H; Smith, W H; Spentzouris, P; Stern, E G; Vakili, M; Vaitaitis, A; V Wu; Yang, U K; J Yu; Zeller, G P; Zimmerman, E D

    arXiv.org, 08/1999
    Paper

    Analyses of structure functions (SFs) from neutrino and muon deep inelastic scattering data have shown discrepancies in F2 for x < 0.1. A new SF analysis of the CCFR collaboration data examining regions in x down to x=.0015 and 0.4 < Q^2 < 1.0 is presented. Comparison to corrected charged lepton scattering results for F2 from the NMC and E665 experiments are made. Differences between muon and neutrino scattering allow that the behavior of F2 from muon scattering could be different from F2 from neutrino scattering as Q^2 approaches zero. Comparisons between F2 muon and F2 neutrino are made in this limit.