Add to ORKG−Pb → pi−pi−pi+Pb′ • • • We do not use the following data for averages, fits, limits, etc. • • • 1243±12±20 1 AUBERT 07AU BABR 10.6 e+ e − → ρ0 ρ±pi ∓ γ 1230–1270 6360 2 LINK 07A FOCS D0 → pi−pi+pi−pi+ 1203 ± 3 3 GOMEZ-DUM...04 RVUE τ+ → pi+pi+pi − ν
G (JPC) = 0+(1 + +) See the Review on “ψ(2S) and χc branching ratios ” before the χc0(1P) Listings
There is a small literature (which we do not try to cover) on this possible narrow state. See KUZNET...
IG (JPC) = 0+(0−+) We have omitted some results that have been superseded by later experiments. The...
1232 ±3 CUTKOSKY 80 IPWA πN → πN 1233 ±2 HOEHLER 79 IPWA πN → πN • • • We do not use the following...
∼ 1400 5 ACHASOV 98H RVUE e+ e − → ωpi+pi− ∼ 1460 6 ACHASOV 98H RVUE e+ e − → K+K− 1440 ± 70 7 CLE...
Seen by ABLIKIM 13X in e+ e − → pi+pi−hc at c.m. energy from 3.90 to 4.42 GeV as a peak in the inva...
2400 ±125 CUTKOSKY 80 IPWA piN → piN 2416 ± 17 HOEHLER 79 IPWA piN → piN 2400 ± 60 HENDRY 78 MPWA pi...
1281.8 ± 0.6 OUR AVERAGE Error includes scale factor of 1.6. See the ideogram below. 1281 ± 2 ± 1 AU...
The data in this block is included in the average printed for a previous datablock. • • • We do no...
2149±17 OUR AVERAGE Includes data from the datablock that follows this one. 2150±40±50 AUBERT 07AU B...
Seen mostly in antinucleon-nucleon annihilation. Needs confirmation in other channels. f2(1565) MASS...
η IG (JPC) = 0+(0−+) We have omitted some results that have been superseded by later experiments. T...
mass and mass difference measurements. VALUE (MeV) DOCUMENT ID TECN CHG COMMENT 2010.27±0.17 OUR FIT...
This entry lists peaks reported in mass spectra around 1560 MeV without implying that they are neces...
G (JPC) = 1−(0−+) We have omitted some results that have been superseded by later experiments. The ...
G (JPC) = 0+(1 + +) See the Review on “ψ(2S) and χc branching ratios ” before the χc0(1P) Listings
There is a small literature (which we do not try to cover) on this possible narrow state. See KUZNET...
IG (JPC) = 0+(0−+) We have omitted some results that have been superseded by later experiments. The...
1232 ±3 CUTKOSKY 80 IPWA πN → πN 1233 ±2 HOEHLER 79 IPWA πN → πN • • • We do not use the following...
∼ 1400 5 ACHASOV 98H RVUE e+ e − → ωpi+pi− ∼ 1460 6 ACHASOV 98H RVUE e+ e − → K+K− 1440 ± 70 7 CLE...
Seen by ABLIKIM 13X in e+ e − → pi+pi−hc at c.m. energy from 3.90 to 4.42 GeV as a peak in the inva...
2400 ±125 CUTKOSKY 80 IPWA piN → piN 2416 ± 17 HOEHLER 79 IPWA piN → piN 2400 ± 60 HENDRY 78 MPWA pi...
1281.8 ± 0.6 OUR AVERAGE Error includes scale factor of 1.6. See the ideogram below. 1281 ± 2 ± 1 AU...
The data in this block is included in the average printed for a previous datablock. • • • We do no...
2149±17 OUR AVERAGE Includes data from the datablock that follows this one. 2150±40±50 AUBERT 07AU B...
Seen mostly in antinucleon-nucleon annihilation. Needs confirmation in other channels. f2(1565) MASS...
η IG (JPC) = 0+(0−+) We have omitted some results that have been superseded by later experiments. T...
mass and mass difference measurements. VALUE (MeV) DOCUMENT ID TECN CHG COMMENT 2010.27±0.17 OUR FIT...
This entry lists peaks reported in mass spectra around 1560 MeV without implying that they are neces...
G (JPC) = 1−(0−+) We have omitted some results that have been superseded by later experiments. The ...
G (JPC) = 0+(1 + +) See the Review on “ψ(2S) and χc branching ratios ” before the χc0(1P) Listings
There is a small literature (which we do not try to cover) on this possible narrow state. See KUZNET...
IG (JPC) = 0+(0−+) We have omitted some results that have been superseded by later experiments. The...