TY - JOUR
T1 - Neutral decay modes of the η0 meson
AU - Devons, S.
AU - Grunhaus, J.
AU - Kozlowski, T.
AU - Nemethy, P.
AU - Shapiro, S.
AU - Horwitz, N.
AU - Kalogeropoulos, T.
AU - Skelly, J.
AU - Smith, R.
AU - Uto, H.
N1 - Funding Information:
Ausl%nder for the organisation of the scanning. The participants from Karlsruhe are indebted to the Bundesministerium fur Wissenschaftliche Forschung for financial support.
PY - 1970
Y1 - 1970
N2 - The branching ratios of the decay of the η0 meson into neutral products have been measured. The η0 is produced in the reaction π-p→η0+n, and the decay products are observed as γ rays by a system of optical spark chambers and counters in nearly 4π geometry. Emphasis was placed on examining evidence for the decay mode η0→π0γγ (→4γ). Measurement of the neutron time of flight in the production process, together with detailed measurement and kinematical analysis of the pictures showing four γ rays, enables us to test each event for consistency with such a decay mode, and also for the "background" process π-+p→2π0+n. From what is essentially a comparison of the observed rates for these processes, we obtain the upper limit for (η0→π0γγ)(η0→all neutrals) ≤7% (90% confidence level), a result which is relatively insensitive to estimates of the efficiency of the detecting system. We also obtain (η0→3π0)(η0→2γ)=0.75±0.09.
AB - The branching ratios of the decay of the η0 meson into neutral products have been measured. The η0 is produced in the reaction π-p→η0+n, and the decay products are observed as γ rays by a system of optical spark chambers and counters in nearly 4π geometry. Emphasis was placed on examining evidence for the decay mode η0→π0γγ (→4γ). Measurement of the neutron time of flight in the production process, together with detailed measurement and kinematical analysis of the pictures showing four γ rays, enables us to test each event for consistency with such a decay mode, and also for the "background" process π-+p→2π0+n. From what is essentially a comparison of the observed rates for these processes, we obtain the upper limit for (η0→π0γγ)(η0→all neutrals) ≤7% (90% confidence level), a result which is relatively insensitive to estimates of the efficiency of the detecting system. We also obtain (η0→3π0)(η0→2γ)=0.75±0.09.
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U2 - 10.1103/PhysRevD.1.1936
DO - 10.1103/PhysRevD.1.1936
M3 - Article
AN - SCOPUS:4243271646
SN - 1550-7998
VL - 1
SP - 1936
EP - 1945
JO - Physical review D: Particles and fields
JF - Physical review D: Particles and fields
IS - 7
ER -