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    The antiproton-nuclei annihilation cross-section at the momentum range from 0.70 to 2.50 GeV/c
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    Using modularized NaI(Tl) detectors, we carried out a high-statistics measurement of inclusive π o and η spectra in antiproton annihilation at rest in a liquid D 2 target. We obtained the following two-meson yields (branching ratios) per \bar p N ( N = p or n ) annihilation: 0.19± 0.09% for π o ω, 1.07±0.19% for π o ρ o , 0.057±0.018% for π o η, 0.0123±0.0055% for π o π o , 0.02±0.02% for π o ρ - , 0.202±0.031% for π o π - , 0.49±0.12% for ηω, 0.45±0.15% for ηρ o , and 0.91±0.22% for ηρ - .
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    Semiclassical transport theory is applied to the pion emission from antiproton annihilation in Ne. In the annihilation of a moving antiproton in nuclei, we find that the leading particle effect is apparent.NUCLEAR REACTIONS Low energy $\overline{p}$-Ne annihilation; pion transport theory; leading particle effect.
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    The range of the proton-antiproton annihilation was calculated for antiproton with energy near 1 Bev. The point is to get the range of pure annihilation interaction, separating the effect of pion production. It was found that the root mean square of this range is given by (1.19\ifmmode\pm\else\textpm\fi{}0.07)\ifmmode\times\else\texttimes\fi{}${10}^{\ensuremath{-}13}$ cm almost independently of the energy.
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    Antiproton
    Annihilation
    Nuclear emulsion
    Branching (polymer chemistry)
    Low energy
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