Can you help with particle physics?

In summary, the conversation discusses the use of lepton universality and lepton-quark symmetry to estimate branching ratios for certain reactions. The first question (a) is deemed not possible without quark mixing, as quarks can only change flavor within their own generation. The second question (b) looks at the ratio of masses between the particles involved. The conversation then delves into the observation of certain processes as evidence for weak neutral currents, with the conclusion that the observation of antielectronneutrino + e- -> antielectronneutrino + e- is not considered unambiguous evidence due to the possibility of the reaction occurring with a W boson.
  • #1
m_ridsdale
I'd really appreciate any help you can give me with the following questions:

Use lepton universality and lepton-quark symmetry (ignore quark mixing) to estimate the branching ratios for:

a) b -> c + e- + anti-electronneutrino
b) tau -> e- + anti-electronneutrino + tauneutrino


Surely (a) is not possible without quark mixing? Isn't it true that without quark mixing, quarks can change flavour but only within their generation, e.g. can have u -> d but not u -> s?

b) I think for this question I just need to look at the ratio of the masses of the mu and the e-, since all differences in their interactions are due to their difference in mass, is this correct? So the answer I would give would be mass(e-)/mass(mu).

Why does observation of the process
antimuneutrino + e- -> antimuneutrino + e-
constitute unambiguous evidence for weak neutral currents, whereas the observation of
antielectronneutrino + e- -> antielectronneutrino + e-
does not?


I've no idea about this, I'd have thought either scattering process could be an electromagnetic interaction; doesn't any interaction involving the Z have an equivalent involving photons?
 
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  • #2
This one's a little advanced for Homework Help. We typically get inclined planes and calculus problems. It will be more likely to get noticed here, in Theoretical Physics.

I'll take a stab at it later.
 
  • #3
Originally posted by m_ridsdale
I'd really appreciate any help you can give me with the following questions:

Use lepton universality and lepton-quark symmetry (ignore quark mixing) to estimate the branching ratios for:

a) b -> c + e- + anti-electronneutrino
b) tau -> e- + anti-electronneutrino + tauneutrino


Surely (a) is not possible without quark mixing? Isn't it true that without quark mixing, quarks can change flavour but only within their generation, e.g. can have u -> d but not u -> s?
agreed.

b) I think for this question I just need to look at the ratio of the masses of the mu and the e-, since all differences in their interactions are due to their difference in mass, is this correct? So the answer I would give would be mass(e-)/mass(mu).
shouldn t it be the ratio of the tau to the electron for this reaction?


Why does observation of the process
antimuneutrino + e- -> antimuneutrino + e-
constitute unambiguous evidence for weak neutral currents, whereas the observation of
antielectronneutrino + e- -> antielectronneutrino + e-
does not?


I've no idea about this, I'd have thought either scattering process could be an electromagnetic interaction; doesn't any interaction involving the Z have an equivalent involving photons?

photons cannot couple to neutral particles. so photons cannot interact with neutrinos.

but i d say the nu_e reaction is not unambiguous evidence for weak neutral currents, because it this reaction could procede with a W boson. not so in the nu_mu case.
 

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