Neutral strange particle production in neutrino and antineutrino charged-current interactions on neon

D. DeProspo, M. Kalelkar, M. Aderholz, H. Akbari, P. P. Allport, V. V. Ammosov, A. Andryakov, A.E. Asratyan, S.K. Badyal, H. C. Ballagh,

Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · 1994 · 25 citations · 16 references

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Abstract

A study has been made of neutral strange particle production in ${\ensuremath{\nu}}_{\mathrm{\ensuremath{\mu}}}$Ne and \ensuremath{\nu}${\mathrm{\ifmmode\bar\else\textasciimacron\fi{}}}_{\mathrm{\ensuremath{\mu}}}$Ne charged-current interactions at a higher energy than any previous study. The experiment was done at the Fermilab Tevatron using the 15-ft. bubble chamber, and the data sample consists of 814(154) observed neutral strange particles from 6263(1115) \ensuremath{\nu}(\ensuremath{\nu}\ifmmode\bar\else\textasciimacron\fi{}) charged-current events. For the \ensuremath{\nu} beam (average event energy 〈${\mathit{E}}_{\ensuremath{\nu}}$〉=150 GeV), the average multiplicities per charged-current event have been measured to be 0.408\ifmmode\pm\else\textpm\fi{}0.048 for ${\mathit{K}}^{0}$, 0.127\ifmmode\pm\else\textpm\fi{}0.014 for \ensuremath{\Lambda}, and 0.015\ifmmode\pm\else\textpm\fi{}0.005 for \ensuremath{\Lambda}\ifmmode\bar\else\textasciimacron\fi{}, which are significantly greater than for lower-energy experiments. The dependence of rates on kinematical variables has been measured, and shows that both ${\mathit{K}}^{0}$ and \ensuremath{\Lambda} production increase strongly with ${\mathit{E}}_{\ensuremath{\nu}}$, ${\mathit{W}}^{2}$, ${\mathit{Q}}^{2}$, and ${\mathit{y}}_{\mathit{B}}$. Compared to lower-energy experiments, single-particle distributions indicate that there is much more ${\mathit{K}}^{0}$ production for ${\mathit{x}}_{\mathit{F}}$>-0.2, and the enhanced \ensuremath{\Lambda} production spans most of the kinematic region. \ensuremath{\Lambda}\ifmmode\bar\else\textasciimacron\fi{} production is mostly in the region \ensuremath{\Vert}${\mathit{x}}_{\mathit{F}}$\ensuremath{\Vert}0.3. The Lund model is shown to be in qualitative agreement with the data, but does not reproduce single-particle distributions in detail. For ${\mathit{x}}_{\mathit{F}}$>-0.2 there is a significant excess of \ensuremath{\Lambda} production over the model's prediction. The \ensuremath{\Lambda} hyperons are found to be polarized in the production plane.

References

16