Recently discovered ZZ diboson

  • Context: Graduate 
  • Thread starter Thread starter Dmitry67
  • Start date Start date
Click For Summary
SUMMARY

The forum discussion centers on the interaction of ZZ dibosons, specifically addressing the mechanisms of their production and decay in high-energy physics experiments. It clarifies that while Z bosons do not interact with themselves, they can interact with W bosons due to the non-commutative nature of the SU(2) x U(1) gauge group structure. The discussion highlights the importance of distinguishing between events where Z bosons decay into different particle types, such as quarks and leptons, to accurately identify their interactions. The Feynman diagram illustrating the process of quark-antiquark annihilation leading to ZZ production is referenced for further clarity.

PREREQUISITES
  • Understanding of gauge theories, specifically SU(2) x U(1) electroweak theory
  • Familiarity with Feynman diagrams and their interpretation in particle physics
  • Knowledge of particle decay processes, particularly Z boson decay channels
  • Basic concepts of high-energy physics experiments and detector technology
NEXT STEPS
  • Study the electroweak theory and its implications on particle interactions
  • Learn about Feynman diagrams and their role in visualizing particle interactions
  • Research the decay channels of Z bosons and their significance in collider experiments
  • Explore the differences between abelian and non-abelian gauge groups in particle physics
USEFUL FOR

Particle physicists, students of high-energy physics, and researchers interested in the electroweak interactions and the behavior of gauge bosons in collider experiments.

Dmitry67
Messages
2,564
Reaction score
1
I know about fermions forming pairs, but I had never heard about the bosons doing it.

Why 2 Z bosons interact (contrary to 2 photons)?
How do we know that we detected 1 ZZ boson, not 2 independent interactions with single Z bosons?
 
Physics news on Phys.org
I presume you are meaning something related to this measurement?

http://www.fnal.gov/pub/today/archive_2008/today08-08-21.html

Nobody has claimed that di-boson production implies a bound state. What is happening is illustrated by the feynman diagram here:

http://www.pd.infn.it/~dorigo/zzdecay.jpg

So you see, the initial fermion line (from quark anti-quark annihilation) radiates two Z bosons, which each in turn decay into whatever Zs can decay into. If each Z decays into the same thing (i.e. you get 4 electrons, 4 muons or 4 quarks), they are difficult to untangle. However, if you look for events where one Z decays to quarks, and the other decays to leptons (i.e. electron or muons, as taus look rather like quark jets), then you can find these events as quark jets and leptons are, generically speaking, detected in different subdetectors of an experiment. I have not mentioned neutrinos as you can't detect these at all (in a colliding HEP experiment at least)...

It is wrong to say that the Z bosons interact with themselves. The Z can, however, interact with the W+ and W-. As to why these gauge bosons can interact and the photon can't is a very interesting one. It boils down to the gauge structure of the underlying theory. The U(1) group of electromagnetism is an abelian group (meaning the generator - the fundamental description of the group - commute, i.e. G(1)G(2) = G(2)G(1)). However, in SU(2) x U(1), the electroweak group structure, the generators no longer commute (i.e. G(1)G(2) != G(2)G(1)). The non-commutation implies self interaction terms are allowed.
 
Thank you for the good explanation!
 
bomanfishwow said:
...

It is wrong to say that the Z bosons interact with themselves. The Z can, however, interact with the W+ and W-. As to why these gauge bosons can interact and the photon can't is a very interesting one. It boils down to the gauge structure of the underlying theory. The U(1) group of electromagnetism is an abelian group (meaning the generator - the fundamental description of the group - commute, i.e. G(1)G(2) = G(2)G(1)). However, in SU(2) x U(1), the electroweak group structure, the generators no longer commute (i.e. G(1)G(2) != G(2)G(1)). The non-commutation implies self interaction terms are allowed.

Actually, the photon can interact with the W+ and W- just like the Z can. The interaction is almost identical, except that the ZWW coupling has an extra factor of \cot\theta_w. Recall that in the electroweak theory, the U(1) of electromagnetism is a subgroup of the full SU(2) x U(1).
 
daschaich said:
Actually, the photon can interact with the W+ and W- just like the Z can. The interaction is almost identical, except that the ZWW coupling has an extra factor of \cot\theta_w. Recall that in the electroweak theory, the U(1) of electromagnetism is a subgroup of the full SU(2) x U(1).

Yes indeed, I was talking explicitly about Z/W interaction terms - I didn't want to get into the fact the U(1)s are different in each case!
 

Similar threads

  • · Replies 4 ·
Replies
4
Views
4K
  • · Replies 2 ·
Replies
2
Views
1K
  • · Replies 4 ·
Replies
4
Views
3K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 1 ·
Replies
1
Views
1K
  • · Replies 17 ·
Replies
17
Views
6K
  • · Replies 10 ·
Replies
10
Views
4K
  • · Replies 2 ·
Replies
2
Views
3K
  • · Replies 5 ·
Replies
5
Views
6K
  • · Replies 13 ·
Replies
13
Views
4K