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.
((a)) Write down the quark content of π−, p and n; the π0 has Q=0, B=0 and S=0. Use these to check that charge, baryon number and strangeness are each conserved across the reaction.
((b)) Assign the isospin I and its third component I3 to π−, p and n from their quark content and to π0 from its place in the pion family, and check that the total I3 of the two incoming particles equals the total I3 of the two outgoing particles.
((c)) The strong interaction is blind to the difference between u and d. Using this blindness, explain in one or two sentences why the pp, pn and nn strong forces are equal (once electric repulsion is removed), and why that same blindness ties the rate of π−p→π0n at s=1232MeV to the rate of π−p→π−p at the same energy.