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33.4 Particles, Patterns, and Conservation Laws

Matter against antimatter, hadrons against leptons, baryons against mesons, and the conserved quantum numbers that decide which decays can happen at all.

College Physics 2e, 33.4 Particles, Patterns, and Conservation Laws

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5 exercises

33.4 Exercise 1

When a π- decays, the products may include:

  1. A positron.
  2. A muon.
  3. A proton.
  4. All of the above.
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33.4 Exercise 12

The π0\pi^{0} is its own antiparticle and decays in the following manner: π0→γ+γ\pi^{0} \rightarrow \gamma + \gamma. What is the energy of each γ\gamma ray if the π0\pi^{0} is at rest when it decays?

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33.4 Exercise 14

The mass of a theoretical particle that may be associated with the unification of the electroweak and strong forces is 1014GeV/c2\text{10}^{\text{14}} \text{GeV}/ c^{2}.

(a) How many proton masses is this?

(b) How many electron masses is this? (This indicates how extremely relativistic the accelerator would have to be in order to make the particle, and how large the relativistic quantity γ\gamma would have to be.)

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33.4 Exercise 16

The decay mode of the positive tau is τ+→μ++νμ+ν-τ\tau^{+ } \rightarrow \mu^{+ } + \nu_{\mu} + \left(\overset{-}{\nu}\right)_{\tau}.

(a) What energy is released?

(b) Verify that charge and lepton family numbers are conserved.

(c) The τ+\tau^{+ } is the antiparticle of the τ−\tau^{- }.Verify that all the decay products of the τ+\tau^{+ } are the antiparticles of those in the decay of the τ−\tau^{- } given in the text.

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33.4 Exercise 18

(a) What is the uncertainty in the energy released in the decay of a π0\pi^{0} due to its short lifetime?

(b) What fraction of the decay energy is this, noting that the decay mode is π0→γ+γ\pi^{0} \rightarrow \gamma + \gamma (so that all the π0\pi^{0} mass is destroyed)?

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Adapted from College Physics © 2022 Rice University. Licensed under CC BY 4.0. Sources: College Physics 2e, College Physics for AP® Courses 2e. Imported at revision f98d7a7.