Consider the strong reaction .

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

Consider the strong reaction π−p→π0n\pi^-p \to \pi^0 n. ((a)) Write down the quark content of π−\pi^-, pp and nn; the π0\pi^0 has Q=0Q=0, B=0B=0 and S=0S=0. Use these to check that charge, baryon number and strangeness are each conserved across the reaction. ((b)) Assign the isospin II and its third component I3I_3 to π−\pi^-, pp and nn from their quark content and to π0\pi^0 from its place in the pion family, and check that the total I3I_3 of the two incoming particles equals the total I3I_3 of the two outgoing particles. ((c)) The strong interaction is blind to the difference between uu and dd. Using this blindness, explain in one or two sentences why the pppp, pnpn and nnnn strong forces are equal (once electric repulsion is removed), and why that same blindness ties the rate of π−p→π0n\pi^-p\to\pi^0n at s=1232 MeV\sqrt{s}=1232\ \mathrm{MeV} to the rate of π−p→π−p\pi^-p\to\pi^-p at the same energy.

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