Determining the type of interaction

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Discussion Overview

The discussion revolves around identifying the type of interaction that occurs when a positive pion interacts with a proton, potentially producing a kaon and another strange particle. Participants explore the implications of conservation laws and the characteristics of the interaction, considering strong and weak nuclear forces.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant asserts that the interaction is a strong interaction based on their experience with recognizing such interactions, but notes the lack of information about the quark composition of the strange particle X complicates the determination.
  • Another participant suggests that if X were a proton, it would indicate a weak interaction, but emphasizes that the probability of this occurring is very low.
  • A different participant points out that the presence of a strange particle implies that X must have non-zero strangeness, leading to the conclusion that X could be a ##\Sigma^{+}##, which would support the idea of a strong interaction if flavor conservation holds.
  • One participant questions the relevance of branching ratios in this context, clarifying that the interaction is a 2-to-2 body scatter, which does not involve branching ratios for proton production.
  • Another participant explores the possibility of X being a ##\Sigma^+## and inquires about the corresponding Feynman diagram, while also questioning whether the mediation particle could be a photon or a Z boson.
  • Responses indicate that while photons or Z bosons could mediate the interaction, gluons are preferred due to their stronger coupling in quark interactions.

Areas of Agreement / Disagreement

Participants express differing views on the type of interaction and the role of conservation laws, with no consensus reached on the exact nature of the interaction or the identity of particle X.

Contextual Notes

The discussion highlights the uncertainty surrounding the quark composition of particle X and the implications of conservation laws on determining the type of interaction. The relevance of branching ratios is also debated, with some participants questioning their applicability in this specific scenario.

maximus123
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Hi everyone,

I have the following question

When a positive pion interacts with a proton, a kaon can be produced, along with another strange particle, as shown in this equation

\pi^++\textrm{P}\longrightarrow \textrm{K}^++\textrm{X}

Circle the type of interaction shown

\textrm{Electromagnetic} \qquad\textrm{gravitational}\qquad\textrm{weak nuclear}\qquad\textrm{strong nuclear}

I know this is a strong interaction as I have gotten used to recognising them. Given a reaction equation, if I was not sure what the interaction type, I would be able to work it out by seeing if the quark composition was conserved. If it was then we have the strong nuclear force. However in the above example. Since we have not been given the quark composition of the X particle, or whether or not its strange particle is strange or antistrange, that is not possible in this case. So how else could I know by looking at the above (incomplete) equation, that it is an example of a strong interaction?

Thanks a lot for any help
 
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It's true that if X is a proton, it would be a weak interaction. But the branching ratio to produce a proton is so small that it probably has never been seen experimentally. You could check on PDG to see if it has been seen, or what the upper limit for it to happen is.
 
maximus123 said:
along with another strange particle

That should tell you that ##X## has non-zero strangeness. To conserve charge and baryon number, ##X## is going to have negative strangeness (regular baryons don't have valence antiquarks) and charge +1, like a ##\Sigma^{+}##. The ##K^{+}## has strangeness +1, so if all the flavour numbers are conserved, this can go as a strong interaction.

I'm not sure why the first reply mentions branching ratios, since this is a ##2 \to 2## body scatter.
 
Just testing my current knowledge- would the particle ##X## be a ##\Sigma^+## ? And would this be the corresponding Feynman diagram?
pion_proton.png

Also, rather than a gluon, could the mediation particle be a photon or ##Z^0##?
 
dukwon said:
I'm not sure why the first reply mentions branching ratios, since this is a 2→22→22 \to 2 body scatter.
because it was confusing. You are right since in that case there is no Branching ratio for proton production (proton is already there).

SnoliF said:
Also, rather than a gluon, could the mediation particle be a photon or Z0Z0Z^0?
quarks prefer interacting with gluons rather than photons (or even worse the massive Z bosons)... so to your question the answer is yes but not as likely.

W's apart from being heavy also have Cabibbo suppressed vertices.
 

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