Chapter 33: Q15CQ (page 1211)
Explain how the weak force can change strangeness by changing quark flavor.
Short Answer
Weak force can change strangeness by decay path \[s \to u + {W^ - }.\]
Chapter 33: Q15CQ (page 1211)
Explain how the weak force can change strangeness by changing quark flavor.
Weak force can change strangeness by decay path \[s \to u + {W^ - }.\]
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Get started for freeThe \[{{\rm{\pi }}^{\rm{0}}}\]is its own antiparticle and decays in the following manner: \[{\pi ^0} \to \gamma + \gamma \]. What is the energy of each \[\gamma \]ray if the \[{\pi ^0}\] is at rest when it decays?
Gluons and the photon are massless. Does this imply that the W+. W- and Z0 are the ultimate carriers of the weak force?
What length track does a \[{{\rm{\pi }}^{\rm{ + }}}\]traveling at 0.100c leave in a bubble chamber if it is created there and lives for \[{\rm{2}}{\rm{.60 \times 1}}{{\rm{0}}^{{\rm{ - 8}}}}{\rm{\;s}}\]? (Those moving faster or living longer may escape the detector before decaying.)
Consider a detector needed to observe the proposed, but extremely rare, decay of an electron. Construct a problem in which you calculate the amount of matter needed in the detector to be able to observe the decay, assuming that it has a signature that is clearly identifiable. Among the things to consider are the estimated half-life (long for rare events), and the number of decays per unit time that you wish to observe, as well as the number of electrons in the detector substance.
Discuss the similarities and differences between the photon and the Z0in terms of particle properties, including forces felt.
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