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G (JPC) = 0+(1 + +) Observed in the radiative decay to Υ(1S, 2S, 3S), therefore C = +. J needs confirmation. χb1(3P) MASS VALUE (MeV) EVTS DOCUMENT ID TECN COMMEN
The J/ψ decay modes f 0 (1270)γ and ρπ have been studied in e + e − collision at 3.1 GeV center of m...
Suggested by some but not all partial-wave analyses across this re-gion. Σ (2080) MASS VALUE (MeV) D...
The J/ψ decay modes f 0 (1270)γ and ρπ have been studied in e + e − collision at 3.1 GeV center of m...
G (JPC) = 0+(1 + +) J needs confirmation. Observed in radiative decay of the Υ(2S), therefore C = +...
G (JPC) = 0+(2 + +) J needs confirmation. Observed in radiative decay of the Υ(3S), therefore C = +...
χb1(1P) I G (JPC) = 0+(1 + +) J needs confirmation. Observed in radiative decay of the Υ(2S), there...
G (JPC) = 0+(1 + +) J needs confirmation. Observed in radiative decay of the Υ(3S), therefore C = +...
G (JPC) = 0+(0 + +) J needs confirmation. Observed in radiative decay of the Υ(3S), therefore C = +...
G (JPC) = 0+(0 + +) J needs confirmation. Observed in radiative decay of the Υ(3S), therefore C = +...
G (JPC) = 0+(2 + +) J needs confirmation. Observed in radiative decay of the Υ(3S), therefore C = +...
G (JPC) = 0+(0 + +) J needs confirmation. Observed in radiative decay of the Υ(2S), therefore C = +...
G (JPC) = 0+(2 + +) J needs confirmation. Observed in radiative decay of the Υ(2S), therefore C = +...
G (JPC) = 0+(1 + +) J needs confirmation. Observed in radiative decay of the Υ(3S), therefore C = +...
h1(1380) I G (JPC) =?−(1 +−) OMITTED FROM SUMMARY TABLE Seen in partial-wave analysis of the K K π ...
G (JPC) = 0+(0 + +) J needs confirmation. Observed in radiative decay of the Υ(2S), therefore C = +...
The J/ψ decay modes f 0 (1270)γ and ρπ have been studied in e + e − collision at 3.1 GeV center of m...
Suggested by some but not all partial-wave analyses across this re-gion. Σ (2080) MASS VALUE (MeV) D...
The J/ψ decay modes f 0 (1270)γ and ρπ have been studied in e + e − collision at 3.1 GeV center of m...
G (JPC) = 0+(1 + +) J needs confirmation. Observed in radiative decay of the Υ(2S), therefore C = +...
G (JPC) = 0+(2 + +) J needs confirmation. Observed in radiative decay of the Υ(3S), therefore C = +...
χb1(1P) I G (JPC) = 0+(1 + +) J needs confirmation. Observed in radiative decay of the Υ(2S), there...
G (JPC) = 0+(1 + +) J needs confirmation. Observed in radiative decay of the Υ(3S), therefore C = +...
G (JPC) = 0+(0 + +) J needs confirmation. Observed in radiative decay of the Υ(3S), therefore C = +...
G (JPC) = 0+(0 + +) J needs confirmation. Observed in radiative decay of the Υ(3S), therefore C = +...
G (JPC) = 0+(2 + +) J needs confirmation. Observed in radiative decay of the Υ(3S), therefore C = +...
G (JPC) = 0+(0 + +) J needs confirmation. Observed in radiative decay of the Υ(2S), therefore C = +...
G (JPC) = 0+(2 + +) J needs confirmation. Observed in radiative decay of the Υ(2S), therefore C = +...
G (JPC) = 0+(1 + +) J needs confirmation. Observed in radiative decay of the Υ(3S), therefore C = +...
h1(1380) I G (JPC) =?−(1 +−) OMITTED FROM SUMMARY TABLE Seen in partial-wave analysis of the K K π ...
G (JPC) = 0+(0 + +) J needs confirmation. Observed in radiative decay of the Υ(2S), therefore C = +...
The J/ψ decay modes f 0 (1270)γ and ρπ have been studied in e + e − collision at 3.1 GeV center of m...
Suggested by some but not all partial-wave analyses across this re-gion. Σ (2080) MASS VALUE (MeV) D...
The J/ψ decay modes f 0 (1270)γ and ρπ have been studied in e + e − collision at 3.1 GeV center of m...