Why can only the weak interaction change quark flavour?

Click For Summary
SUMMARY

The weak interaction is the only fundamental force capable of changing quark flavor due to its unique properties involving the W boson, which is electrically charged. Other interactions, such as electromagnetic and strong forces, do not account for the differences in quark charges or weak charge values. The discussion emphasizes that while the W boson facilitates flavor changes, the Z boson does not, as it is electrically neutral. Additionally, the concept of electroweak symmetry breaking is crucial in understanding these interactions.

PREREQUISITES
  • Understanding of weak interactions and their role in particle physics
  • Familiarity with gauge bosons, specifically W and Z bosons
  • Knowledge of quark flavors and their associated quantum numbers
  • Basic principles of electroweak symmetry breaking
NEXT STEPS
  • Study the role of W and Z bosons in the Standard Model of particle physics
  • Explore the concept of electroweak symmetry breaking in detail
  • Learn about quark flavor mixing and the CKM matrix
  • Investigate gauge field theories and their implications in particle interactions
USEFUL FOR

Students of particle physics, physicists specializing in the Standard Model, and anyone interested in the mechanisms of fundamental interactions and quark behavior.

AlanKirby
Messages
20
Reaction score
0
Hi there, so my question is as follows.

I understand that only the weak interaction can change the flavour of a quark, but why?

Idea 1: It's due to the change in flavour also meaning a change in mass, thus a massive exchange particle is needed (gravity is negligible so forget the massive graviton). But then since the exchange particles are themselves virtual, could a photon for example, not simply be 'off mass shell' and produce the same result?

Idea 2: It's to do with a change in electric charge (assuming we always deal with U,C,T to S,B,D quarks flavours or vice versa, which i don't know if that is true), thus an electrically charged exchange particle is needed, i.e. W boson (and hence Z boson doesn't cause a change in quark flavour since it's electrically neutral)?

Idea 3: The different quark flavours have a different value of weak charge (which is a different quantum number), thus to change this from one value to another requires an exchange particle with weak charge, thus the W bosons are the only gauge bosons that can cause this flavour change (and again, thus the Z boson cannot since it has no weak charge)?

I'm sure that someone is about to confuse me with some gauge field theory stuff, but I would appreciate an answer, despite how confusing it may seem to an undergrad such as myself.

Thank you kindly for any response.
 
Physics news on Phys.org
Weak interactions are the only interactions whichd deal with the SU(2) doublets containing quarks with different charges. All other interactions are blind to this difference. In essence, it is akin to asking why only strong interactions can change the colour of a quark with the addition that electroweak symmetry breaking makes the W charged under the residual U(1) symmetry, i.e., electromagnetism.
 
  • Like
Likes   Reactions: AlanKirby
Orodruin said:
Weak interactions are the only interactions whichd deal with the SU(2) doublets containing quarks with different charges. All other interactions are blind to this difference. In essence, it is akin to asking why only strong interactions can change the colour of a quark with the addition that electroweak symmetry breaking makes the W charged under the residual U(1) symmetry, i.e., electromagnetism.
Thank you for your response. Can I please ask for a recommended text for this material, preferably an introductory text and then separately a more advanced text.

Thanks again.
 
AlanKirby said:
Idea 1: It's due to the change in flavour also meaning a change in mass, thus a massive exchange particle is needed (gravity is negligible so forget the massive graviton). But then since the exchange particles are themselves virtual, could a photon for example, not simply be 'off mass shell' and produce the same result?
This has nothing to do with masses.
A hypothetical graviton would be massless.
AlanKirby said:
Idea 2: It's to do with a change in electric charge (assuming we always deal with U,C,T to S,B,D quarks flavours or vice versa, which i don't know if that is true), thus an electrically charged exchange particle is needed, i.e. W boson (and hence Z boson doesn't cause a change in quark flavour since it's electrically neutral)?
The W boson is the only boson with electric charge, but you could have changes like charm->up or muon->tau with uncharged bosons. It is easy to allow a boson to mediate those interactions, but we never observed those interactions.
 
  • Like
Likes   Reactions: AlanKirby
mfb said:
This has nothing to do with masses.
A hypothetical graviton would be massless.
The W boson is the only boson with electric charge, but you could have changes like charm->up or muon->tau with uncharged bosons. It is easy to allow a boson to mediate those interactions, but we never observed those interactions.
Thanks for your response. So are you suggesting that 'idea 2' is the correct way to be thinking about it on a simple level?
 
Well, charge conservation tells you "up -> down + photon" is impossible. It does not tell you "charm -> up + photon" is impossible.
 
  • Like
Likes   Reactions: AlanKirby

Similar threads

  • · Replies 23 ·
Replies
23
Views
4K
  • · Replies 8 ·
Replies
8
Views
3K
  • · Replies 5 ·
Replies
5
Views
1K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 11 ·
Replies
11
Views
2K
  • · Replies 4 ·
Replies
4
Views
4K
  • · Replies 4 ·
Replies
4
Views
3K
  • · Replies 8 ·
Replies
8
Views
2K
  • · Replies 6 ·
Replies
6
Views
2K
Replies
7
Views
2K