Add to ORKGSeen 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 invariant mass distribution of the hc pi ± system. Needs confirmation
µ J = 12 µ MASS (atomic mass units u) The muon’s mass is obtained from the muon-electron mass ratio ...
Seen mostly in antinucleon-nucleon annihilation. Needs confirmation in other channels. f2(1565) MASS...
Seen in the Λ+c π ± mass spectrum. The natural assignment is that this is the JP = 3/2+ excitation o...
Seen as a peak in the invariant mass distribution of the J/ψpi± system by BES3 (ABLIKIM 13T) in e+ e...
−Pb → pi−pi−pi+Pb′ • • • We do not use the following data for averages, fits, limits, etc. • • • ...
We have set an upper limit on the mass from a study of the four-pion invariant-mass distribution in ...
∼ 1400 5 ACHASOV 98H RVUE e+ e − → ωpi+pi− ∼ 1460 6 ACHASOV 98H RVUE e+ e − → K+K− 1440 ± 70 7 CLE...
This entry lists peaks reported in mass spectra around 1560 MeV without implying that they are neces...
Seen by BHARDWAJ 13 in B → χc1γK decays as a narrow peak in the invariant mass distribution of the χ...
We list here three different peaks with close masses and widths seen in the mass distributions of ωω...
We present \u3c0+\u3c0 12 invariant-mass distributions between 300 and 380 MeV for the 2H, 4He, 16O,...
Seen in antinucleon-nucleon annihilation at rest. Needs confirma-tion. f2(1565) MASS VALUE (MeV) DOC...
Using 342 fb−1 of e+e − annihilation data collected with the BABAR detector at the SLAC PEP-II elect...
The c-quark mass corresponds to the “running ” mass mc (µ = mc) in the MS scheme. We have converted ...
We report on a study of the process e+ e- → π± (DD*)? at sqrt[s] = 4.26??GeV using a 525?pb(-1) data...
µ J = 12 µ MASS (atomic mass units u) The muon’s mass is obtained from the muon-electron mass ratio ...
Seen mostly in antinucleon-nucleon annihilation. Needs confirmation in other channels. f2(1565) MASS...
Seen in the Λ+c π ± mass spectrum. The natural assignment is that this is the JP = 3/2+ excitation o...
Seen as a peak in the invariant mass distribution of the J/ψpi± system by BES3 (ABLIKIM 13T) in e+ e...
−Pb → pi−pi−pi+Pb′ • • • We do not use the following data for averages, fits, limits, etc. • • • ...
We have set an upper limit on the mass from a study of the four-pion invariant-mass distribution in ...
∼ 1400 5 ACHASOV 98H RVUE e+ e − → ωpi+pi− ∼ 1460 6 ACHASOV 98H RVUE e+ e − → K+K− 1440 ± 70 7 CLE...
This entry lists peaks reported in mass spectra around 1560 MeV without implying that they are neces...
Seen by BHARDWAJ 13 in B → χc1γK decays as a narrow peak in the invariant mass distribution of the χ...
We list here three different peaks with close masses and widths seen in the mass distributions of ωω...
We present \u3c0+\u3c0 12 invariant-mass distributions between 300 and 380 MeV for the 2H, 4He, 16O,...
Seen in antinucleon-nucleon annihilation at rest. Needs confirma-tion. f2(1565) MASS VALUE (MeV) DOC...
Using 342 fb−1 of e+e − annihilation data collected with the BABAR detector at the SLAC PEP-II elect...
The c-quark mass corresponds to the “running ” mass mc (µ = mc) in the MS scheme. We have converted ...
We report on a study of the process e+ e- → π± (DD*)? at sqrt[s] = 4.26??GeV using a 525?pb(-1) data...
µ J = 12 µ MASS (atomic mass units u) The muon’s mass is obtained from the muon-electron mass ratio ...
Seen mostly in antinucleon-nucleon annihilation. Needs confirmation in other channels. f2(1565) MASS...
Seen in the Λ+c π ± mass spectrum. The natural assignment is that this is the JP = 3/2+ excitation o...