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Mesic molecular effects in the capture of negative pions stopped in gaseous hydrogen isotopes
25
Citations
17
References
1983
Year
Mesic Molecular EffectsNuclear PhysicsEngineeringHadron PhysicNuclear DataMolecular BiologyChemistryNuclear MaterialsLepton-nucleon ScatteringNuclear DecayBiophysicsNegative PionsHigh-energy Nuclear ReactionPhysicsNuclear TheoryAtomic PhysicsHydrogenNuclear Capture ProbabilityExperimental Nuclear PhysicsNatural SciencesParticle PhysicsProton TransferGaseous Hydrogen IsotopesShort-range CorrelationsMeson SpectroscopyStopped PionsHd Gas
The influence of molecular structure on the nuclear capture probability of stopped negative pions has been observed by comparing the ${\ensuremath{\pi}}^{0}$ gamma-ray spectrum from ${\ensuremath{\pi}}^{\ensuremath{-}}$ mesons stopped in HD gas to that from a mixture of equal amounts of ${\mathrm{H}}_{2}$ plus ${\mathrm{D}}_{2}$. The fraction of stopped pions that are captured by a proton in the ${\mathrm{H}}_{2}$+${\mathrm{D}}_{2}$ mixture is ${f}_{{\mathrm{H}}_{2}{\mathrm{D}}_{2}}=0.417\ifmmode\pm\else\textpm\fi{}0.004$, while for HD it is ${f}_{\mathrm{HD}}=0.338\ifmmode\pm\else\textpm\fi{}0.008$, independent of the gas pressure between 6 and 90 atm. The ratio, $\frac{{f}_{{\mathrm{H}}_{2}{\mathrm{D}}_{2}}}{{f}_{\mathrm{HD}}}$, of the fractions is 1.23\ifmmode\pm\else\textpm\fi{}0.03.
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