Strong, weak, electromagnetic interactions

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Homework Help Overview

The discussion revolves around particle interactions, specifically distinguishing between strong, weak, and electromagnetic interactions in various decay reactions involving hadrons and leptons. The original poster expresses confusion regarding the classification of specific reactions based on conservation laws and the types of particles involved.

Discussion Character

  • Conceptual clarification, Assumption checking, Problem interpretation

Approaches and Questions Raised

  • The original poster attempts to classify several particle decay reactions, questioning why certain reactions are categorized as weak or electromagnetic despite involving only hadrons or leptons. They raise specific examples and inquire about conservation laws, such as strangeness and isospin.

Discussion Status

Participants are engaging with the original poster's questions, offering insights into isospin and the nature of weak interactions. Some suggest that certain reactions can proceed via multiple interaction types, while others emphasize the importance of conservation laws in determining the interaction type. There is an ongoing exploration of the complexities involved in classifying these reactions.

Contextual Notes

There are mentions of potential misunderstandings regarding isospin and the conservation of strangeness, as well as the original poster's uncertainty about the accuracy of the reactions presented. The discussion reflects a learning environment where assumptions and definitions are being critically examined.

genloz
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Homework Statement


I had a whole list of reactions and had to show whether or not they could occur... I understood most of the reasons, bar the following, but was more confused about whether or not a reaction was strong or weak... I know that if the reaction involves a lepton its weak, and if it involves a photo, it's electromag, but baryons alone don't define whether a reaction is strong or weak:
For example:

\Sigma^{-} \rightarrow n + \pi^{-}
I understand strangeness is not conserved, but why is it a weak interaction if it only involves hadrons?

e^{+} + e^{-} \rightarrow \mu^{+} + \mu^{-}
Why is this an electromag reaction when only leptons are involved and charge is conserved on both sides and no photons are involved? Shouldn't it be a weak?

K^{-} \rightarrow \pi^{-} + \pi^{0}
This only involves hadrons and strangeness isn't conserved, so should this be an impossible strong reaction?
I thought weak decays only didn't conserve partity, but the answers say this is a possible weak decay, does that mean weak decays don't need to conserve strangeness either? Also why is it weak rather than strong?

\pi^{-} + p \rightarrow \Lambda^{-} + \K^{0}
I thought this would be prevented due to lack of strangeness conservation, but it's allowed via the strong interaction, why?

Thanks very much!
 
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\Sigma^{-} \rightarrow n + \pi^{-}

Have you checked isospin and 3-component of isospin? It can be a weak, if it is done by a W boson. The general rule you are referring to that if neutrinos are emitted, then it is weak, don't go the reverse way, it is not equivalence. All neutrinos comes from weak, but not all weak produces neutrinos. So you must give up this thinking, same holds for the EM interaction.

e^{+} + e^{-} \rightarrow \mu^{+} + \mu^{-}
can proceed both by virtual photon and Z-boson, i.e it can do both weak and EM, but weak is ... weak = unlikley, so the observed muons comes from EM interaction in like 99.99999999999999999999999999999999999% of the cases.

K^{-} \rightarrow \pi^{-} + \pi^{0}
Strangeness is not conserved right? So it is a weak.
Also: Check isopspin and 3-component of isospin.


\pi^{-} + p \rightarrow \Lambda^{-} + K^{0}

I have never heard of Lambda minus baryon.. you must mean lamda zero (charge is not concerved otherwise)
Lamda-0 has one strange quark, and K-0 has one anti-strange quark, so total strangeness is conserved.
Please check if you wrote this reaction correct before proceeding altough.
 
Last edited:
pi- I:1 I3:1 Tz: ??
pi0 I:1 I3:0 Tz: ??
n I:1/2 I3:1/2 Tz:uud 1/2-1/2-1/2:-1/2
K- ubar s I: 1/2+0:1/2 I3:-1/2+0: -1/2 Tz: ??
Sigma- dds I:1/2+1/2+0:1 I3:-1/2+-1/2+0:-1 Tz: -1/2-1/2-1/2
Tz: u c t neutrinos 1/2
Tz: d s b charged leptons -1/2So
\Sigma^{-} \rightarrow n + \pi^{0}{/tex]<br /> I: 1 -&gt; 1/2 + 1 not conserved<br /> I3: -1 -&gt; 1/2 + 0 not conserved<br /> Tz: not sure<br /> <br /> K^{-} \rightarrow \pi^{-} + \pi^{0}{/tex]&lt;br /&gt; I: 1/2 -&amp;gt; 1 + 1 not conserved&lt;br /&gt; I3: -1/2 -&amp;gt; 1 + 0 not conserved&lt;br /&gt; Tz: not sure&lt;br /&gt; &lt;br /&gt; Whcih still doesn&amp;#039;t make sense...
 
You don't know what isospin and third component of isospin is? Look it up. i can't help you with that.

I don't understand what you have written... just a mess, neutrinos don't have isospin etc..

Aslo check the thing i wrote to you regarding last reaction with that lamda minus of yours.
 

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