par Wittek, Wolfgang;Adeholz, M.;Schmitz, Norbert;Guy, J. G V;Cooper-Sarkar, Amanda A.M.;Venus, W.;Allport, Phil;Wells, James;Baton, J.P.;Kasper, Penelope;Neveu, Magella;Berggren, Mikael;Hulth, Per Olof;Bertrand, Daniel
;Marage, Pierre
;Sacton, Jean
;Brisson, Violette;Petiau, P.;Vallée, Claude;Bullock, Frederick;Fitch, P.J.;Sansum, R.A. R.A.;Simopoulou, E.;Burkot, W;Coghen, T.;Calicchio, Marco;Erriquez, Onofrio;Fogli-Muciaccia, M.T.;Clayton, E.F. E.F.;Miller, Dave;Mobayyen, M.M. M.M.;Jones, G.T.;Middleton, Robin R.P.;O'Neale, S.;Varvell, Kevin K.E.;Klein, Harold;Morrison, Douglas R O;Parker, Monique
;Wachsmuth, H.;Vayaki, A.
Référence Physics letters. Section B, 187, 1-2, page (179-184)
Publication Publié, 1987-03




Référence Physics letters. Section B, 187, 1-2, page (179-184)
Publication Publié, 1987-03
Article révisé par les pairs
Résumé : | In a bubble chamber experiment with BEBC the spin alignment parameter η= 1 2 (2ρ{variant}00 - ρ{variant}11 - ρ{variant}-1-1) is measured for ρ{variant}0 mesons produced in deep inelastic charged-current antineutrino and neutrono interactions on neon. In the current fragmentation region η is found to be ηv=0.48±0.27 (stat.)±0.15 (syst.) for vNe and ηv=0.12±0.20 (stat.)±0.10 (syst.) for vNe interactions. © 1987. |