What Fundamental Interactions Govern These Elementary Particle Processes?

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Homework Help Overview

The discussion revolves around identifying the fundamental interactions responsible for various elementary particle processes, including weak decay, baryon number conservation, and pair production. The context is particle and nuclear physics, with the original poster seeking clarification on their reasoning regarding these interactions.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants explore the validity of the original poster's deductions about the interactions involved in specific particle processes. Questions arise regarding the conservation laws and the conditions necessary for certain interactions to occur.

Discussion Status

Some participants provide feedback on the original poster's reasoning, suggesting that certain conservation laws are not sufficient to justify the processes. There is an ongoing examination of the assumptions made about lepton number conservation and the requirement for additional particles to conserve momentum and energy.

Contextual Notes

The original poster identifies as a beginner in particle and nuclear physics, which may influence their understanding of the concepts discussed. There is a focus on clarifying the definitions and implications of fundamental interactions in the context of the given processes.

sudipmaity
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Homework Statement


Indicate the fundamental interactions through which the following processes occur.Justify.
n -> p+ e- + -νe...1
p+p -> p+p+n+-n...2
π+ -> μ++ -νμ...3
γ -> e+ + e-...4

Homework Equations

The Attempt at a Solution


1... is possible due to weak decay .electron antineutrino production.
2... is possible due to baryon no. conservation.
3... is not possible as lepton no. is not conserved.
4...is possible due to pair production and if energy of gamma rays is greater than 1.02MeV.It has been expermentally proven.
Are my deductions correct?? I am a particle, nuclear physics beginner.[/B]
 
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Assuming that -ve means ##\bar\nu_e## etc. The first three are fine as long as the protons in (2) have enough CoM energy to create the neutron-antineutron pair.

For (4), it is not possible unless you can transfer momentum from an external field, such as that of a nearby nucleus. As it stands, you cannot conserve energy and momentum at the same time.
 
sudipmaity said:
1... is possible due to weak decay .electron antineutrino production.
2... is possible due to baryon no. conservation.
3... is not possible as lepton no. is not conserved.
4...is possible due to pair production and if energy of gamma rays is greater than 1.02MeV.It has been expermentally proven.
Are my deductions correct?? I am a particle, nuclear physics beginner.[/B]
You don't seem to be answering the question, which is to identify which interaction is responsible for each process.

For #2, I wouldn't say conservation of baryon number makes it possible. Conservation laws are generally used to rule out potential processes.

For #3, you need to recognize that the antineutrino has a lepton number of -1 because it's antimatter.

For #4, you need a second photon to be able to conserve momentum and energy. This second photon could be a virtual photon associated with the external field Orodruin mentions.
 
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Thank you vela.Is my answer to to #1 correct??
 
You tell me. Why do you think it's mediated by the weak interaction?
 

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