Problem 21
Question
In which of the following decays are the three lepton numbers conserved? In each case, explain your reasoning. (a) \(\mu^{-} \rightarrow \mathrm{e}^{-}+\nu_{\mathrm{e}}+\overline{\nu}_{\mu} ;(\mathrm{b}) \tau^{-} \rightarrow \mathrm{e}^{-}+\overline{\nu}_{\mathrm{e}}+\nu_{\tau} ;(\mathrm{c}) \pi^{+} \rightarrow \mathrm{e}^{+}+\overline{\gamma}\) \((\mathrm{d}) \mathrm{n} \rightarrow \mathrm{p}+\mathrm{e}^{-}+\overline{\nu}_{\mathrm{e}}\)
Step-by-Step Solution
Verified Answer
Decays (a), (b), and (d) conserve lepton numbers; decay (c) does not.
1Step 1: Define Lepton Numbers
Leptons are assigned lepton numbers based on their generation: electron (
ue), muon (
umu), and tau (
utau). Each has its own lepton number, and for anti-leptons, the lepton number is negative. A process conserves lepton numbers if the sum of electron, muon, and tau lepton numbers is the same before and after.
2Step 2: Evaluate Process (a)
In the decay \(\mu^{-} \rightarrow \mathrm{e}^{-} + u_{\mathrm{e}} + \overline{u}_{\mu}\), the lepton numbers are: muon: -1 (\(\mu^{-}\)) to -1 (\(\overline{u}_{\mu}\)), electron: 0 to +1 (\(\mathrm{e}^{-}\) and \(u_{\mathrm{e}}\)). All lepton numbers remain balanced, as electron number goes from 0 to +1, muon is conserved -1 to -1, and tau is unchanged at 0.
3Step 3: Evaluate Process (b)
In the decay \(\tau^{-} \rightarrow \mathrm{e}^{-} + \overline{u}_{\mathrm{e}} + u_{\tau}\), the lepton numbers are: tau: -1 (\(\tau^{-}\)) to -1 (\(u_{\tau}\)), electron: 0 to +1 (\(\mathrm{e}^{-}\)) and -1 (\(\overline{u}_{\mathrm{e}}\)). All lepton numbers are conserved in this process.
4Step 4: Evaluate Process (c)
In the decay \(\pi^{+} \rightarrow \mathrm{e}^{+} + \overline{\gamma}\), the initial state \(\pi^{+}\) is a hadron with no lepton numbers. The final state should have the same total lepton number. However, \(\mathrm{e}^{+}\) has an electron lepton number of -1, and there is no compensating lepton produced, violating lepton number conservation.
5Step 5: Evaluate Process (d)
In the decay \(\mathrm{n} \rightarrow \mathrm{p} + \mathrm{e}^{-} + \overline{u}_{\mathrm{e}}\), the lepton numbers are: initial (n) has no lepton number, electron lepton number goes from 0 to +1 (\(\mathrm{e}^{-}\)) and -1 (\(\overline{u}_{\mathrm{e}}\)), ensuring conservation of electron lepton number. Other lepton numbers remain unchanged.
Key Concepts
Lepton Decay ProcessesParticle PhysicsMuon DecayTau DecayParticle Interaction
Lepton Decay Processes
Lepton decay processes are fundamental events in particle physics where a heavier lepton transforms into lighter particles, often involving neutrinos. A crucial aspect of these processes is lepton number conservation. Each type of lepton, such as electrons, muons, and tau particles, is assigned a lepton family number. This number remains conserved in a closed system.
- In a decay process, the sum of lepton numbers before decay must equal the sum after decay.
- For electrons ( ue), the electron lepton number is conserved.
- For muons ( umu), the muon lepton number remains unchanged.
- For tau particles ( utau), the tau lepton number is preserved.
Particle Physics
Particle physics is the branch of science that studies the smallest building blocks of the universe and the interactions between them. It's concerned with particles like quarks, leptons, and gauge bosons. Lepton decay processes fall under this realm as they involve fundamental particles like electrons, muons, and taus.
Particle physics establishes conservation laws like those of energy, momentum, and importantly, lepton number.
Particle physics establishes conservation laws like those of energy, momentum, and importantly, lepton number.
- Conservation laws are pivotal, as they guide understanding of allowed and forbidden particle interactions.
- Experiments in particle physics probe these interactions, often using accelerators to collide particles at high energies.
Muon Decay
Muon decay is an exemplary lepton decay process where a muon (mu) transforms into an electron (e) with associated neutrinos. In particle physics, the decay is generally represented by:\[ egin{align*} ext{Process:} \,
ightarrow ext{e}^- + u_e + ar{u}_u ext{Checks:} ext{Conservation of:} \ ext{Pic}\ ext{Mud}\ ext{MudD \} ext{Before:} u =Ker, eut=0\ ext{Invalid\}} ext{Checks:}\]One of the definitive attributes of particle decay is conservation law adherence. Every muon's signature has a Lepton number of \(-1\).\The resulting particles must match these quantities and therefore maintain a balanced muon number across columns\( ext{-1 for N'} observations\).={
Tau Decay
Tau decay is another lepton decay process involving the transformation of a tau lepton into lighter particles. The decay usually results in an electron or muon, along with associated neutrinos:\[ au^-
ightarrow ext{e}^- + ar{u}_e + u_ au \] In this decay, -1 comes from tau (tau), balanced by +1 for electrons and -1 for neutrinos. \The system comes into Place 1 with Property Record Decimal digits of -\(1/N\)\.Key features include:
- Conservation is essential: Each chain of resulting transformations must meet equality checks\.
- Observe Lepton Interaction: Leptons returning may behave in forms without \(\demoteform\u_}\)\.
Particle Interaction
Particle interaction involves how particles exchange energy and momentum and how it affects their behavior. In particle physics, interactions are generally categorized based on the force responsible, such as electromagnetic, weak, or strong forces. Lepton decay processes are primarily governed by the weak nuclear force.
The weak force facilitates the transformation of one type of lepton into another, often accompanied by neutrinos.
The weak force facilitates the transformation of one type of lepton into another, often accompanied by neutrinos.
- Interactions explain decay pathways and particle transformations.
- The weak force allows charged and neutral current interactions, critical in lepton decays.
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