Near the pion-production threshold

PHYSICS · Multi-part · Fermi University Physics · Particle Physics & Quantum Fields · Symmetry, groups and the quark model · Symmetry, groups and the quark model

Particle Physics, Ch Isospin: a symmetry used as bookkeeping

Problem

Near the pion-production threshold, two nucleons can fuse into a deuteron and a single pion: pp→dπ+,np→dπ0.pp \to d\pi^+, \qquad np \to d\pi^0. The deuteron dd is the bound state of a proton and a neutron and carries isospin I=0I=0. The pion carries I=1I=1, so the isospin of the final state dπd\pi is fixed at I=1I=1, whatever the pion's charge. The two-nucleon initial states decompose in isospin as follows (quoted): the pppp state is purely I=1I=1, so it reaches the I=1I=1 final state with probability 11; the npnp state is I=1I=1 with probability 12\tfrac12 and I=0I=0 with probability 12\tfrac12, and only its I=1I=1 part can reach the dπd\pi channel. ((a)) Using these quoted probabilities, predict the ratio of reaction rates pp→dπ+:np→dπ0pp\to d\pi^+ : np\to d\pi^0. ((b)) In a bubble-chamber exposure under identical beam conditions, 850850 examples of pp→dπ+pp\to d\pi^+ and 460460 examples of np→dπ0np\to d\pi^0 are counted. Compute the measured ratio and compare it with the prediction.

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