1232 ±3 CUTKOSKY 80 IPWA πN → πN 1233 ±2 HOEHLER 79 IPWA πN → πN • • • We do not use the following data for averages, fits, limits, etc. • •
2205 ± 10 HOEHLER 79 IPWA πN → πN 2300 ±100 HENDRY 78 MPWA πN → πN • • • We do not use the followi...
Older results have been retained simply because there is little infor-mation at all about this possi...
The data in this block is included in the average printed for a previous datablock. • • • We do no...
1232 ±3 CUTKOSKY 80 IPWA πN → πN 1233 ±2 HOEHLER 79 IPWA πN → πN • • • We do not use the following...
1650 ±30 CUTKOSKY 80 IPWA πN → πN 1670 ± 8 HOEHLER 79 IPWA πN → πN • • • We do not use the followi...
2400 ±125 CUTKOSKY 80 IPWA piN → piN 2416 ± 17 HOEHLER 79 IPWA piN → piN 2400 ± 60 HENDRY 78 MPWA pi...
1485.0 ± 1.2 ARNDT 06 DPWA piN → piN, ηN 1440 ±30 CUTKOSKY 80 IPWA piN → piN 1410 ±12 HOEHLER 79 IPW...
This entry was previously called U1(2400). See also ρ(2150), f2(2150), ρ3(2250), f4(2300). ρ5(2350) ...
−Pb → pi−pi−pi+Pb′ • • • We do not use the following data for averages, fits, limits, etc. • • • ...
1281.8 ± 0.6 OUR AVERAGE Error includes scale factor of 1.6. See the ideogram below. 1281 ± 2 ± 1 AU...
p MASS (atomic mass units u) The mass is known much more precisely in u (atomic mass units) than in ...
mass and mass difference measurements. VALUE (MeV) DOCUMENT ID TECN CHG COMMENT 2010.27±0.17 OUR FIT...
tripling the scaling S-factors applied to the uncertainties to account for model-dependence, handlin...
2300±100 HENDRY 78 MPWA πN → πN • • • We do not use the following data for averages, fits, limits,...
G (JPC) = 0+(1 + +) See the Review on “ψ(2S) and χc branching ratios ” before the χc0(1P) Listings
2205 ± 10 HOEHLER 79 IPWA πN → πN 2300 ±100 HENDRY 78 MPWA πN → πN • • • We do not use the followi...
Older results have been retained simply because there is little infor-mation at all about this possi...
The data in this block is included in the average printed for a previous datablock. • • • We do no...
1232 ±3 CUTKOSKY 80 IPWA πN → πN 1233 ±2 HOEHLER 79 IPWA πN → πN • • • We do not use the following...
1650 ±30 CUTKOSKY 80 IPWA πN → πN 1670 ± 8 HOEHLER 79 IPWA πN → πN • • • We do not use the followi...
2400 ±125 CUTKOSKY 80 IPWA piN → piN 2416 ± 17 HOEHLER 79 IPWA piN → piN 2400 ± 60 HENDRY 78 MPWA pi...
1485.0 ± 1.2 ARNDT 06 DPWA piN → piN, ηN 1440 ±30 CUTKOSKY 80 IPWA piN → piN 1410 ±12 HOEHLER 79 IPW...
This entry was previously called U1(2400). See also ρ(2150), f2(2150), ρ3(2250), f4(2300). ρ5(2350) ...
−Pb → pi−pi−pi+Pb′ • • • We do not use the following data for averages, fits, limits, etc. • • • ...
1281.8 ± 0.6 OUR AVERAGE Error includes scale factor of 1.6. See the ideogram below. 1281 ± 2 ± 1 AU...
p MASS (atomic mass units u) The mass is known much more precisely in u (atomic mass units) than in ...
mass and mass difference measurements. VALUE (MeV) DOCUMENT ID TECN CHG COMMENT 2010.27±0.17 OUR FIT...
tripling the scaling S-factors applied to the uncertainties to account for model-dependence, handlin...
2300±100 HENDRY 78 MPWA πN → πN • • • We do not use the following data for averages, fits, limits,...
G (JPC) = 0+(1 + +) See the Review on “ψ(2S) and χc branching ratios ” before the χc0(1P) Listings
2205 ± 10 HOEHLER 79 IPWA πN → πN 2300 ±100 HENDRY 78 MPWA πN → πN • • • We do not use the followi...
Older results have been retained simply because there is little infor-mation at all about this possi...
The data in this block is included in the average printed for a previous datablock. • • • We do no...