How does the Z boson obtain its mass of 90 GeV?

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Homework Help Overview

The discussion revolves around the mass of the Z boson, specifically its mass of 90 GeV, and the associated production peaks of various quarks in the context of particle physics. Participants explore the factors influencing quark production and the characteristics of particles at different energy levels.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants discuss the vertex and propagator factors related to particle interactions, the calculation of R, and the significance of energy peaks at 3 GeV, 10 GeV, and 100 GeV. Questions arise regarding the restrictions on quark formation and the implications of the mass of the Z boson compared to other particles.

Discussion Status

The discussion is ongoing, with participants providing insights into the production of different quarks and their associated energy levels. Some participants suggest that the peaks correspond to specific mesons, while others question the relationship between quark masses and the formation of hadrons. There is a recognition of the Z boson as an elementary particle, but the inquiry into its mass remains unresolved.

Contextual Notes

Participants note that not all quarks can be produced at lower energy levels, and there are specific ranges for quark production. The discussion also highlights the decay of the top quark and its implications for hadron formation, as well as the absence of particles with mass 45 GeV in the context of the Z boson.

unscientific
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Homework Statement



(a) What are their vertex and propagator factors?
(b) Find the value of R.
(c) Explain the peaks at 3, 10 and 100 GeV.

quarkproduction1.png


Homework Equations

The Attempt at a Solution



Part (a)
They have the same propagator factor ##\frac{1}{P \cdot P}##.
Vertex factor for muon production is ##(1)(-1)g_{EM}^2 = -g_{EM}^2##.
Vertex factor for hadron production is ##\sum -q^2##.

Part (b)
In the rage of 2GeV to 20GeV, types of quarks produced: u,d,s,c,b.

R = 3 \times \frac{e^2\left( -\frac{4}{9} -\frac{1}{9} - \frac{1}{9} - \frac{4}{9} - \frac{1}{9} \right)}{-e^2} = \frac{11}{3}

Factor of 3 comes from the 3 colours, R, G and B.

Part (c)
Masses of quarks: u, d ~ ##10^{-3} GeV##, s~ ##0.1GeV##, c~##1 GeV##, b~##4eV##, t~##170GeV##.

Peak at 3GeV comes from production of charmed quarks.
Peak at 10GeV comes from production of bottom quarks.
Peak at 100GeV comes from production of top quarks.
 
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unscientific said:
In the rage of 2GeV to 20GeV, types of quarks produced: u,d,s,c,b.
Not all of them are possible over the full range of 2 to 20 GeV.
unscientific said:
Peak at 3GeV comes from production of charmed quarks.
Peak at 10GeV comes from production of bottom quarks.
Not the general production, that leads to the flat R you calculated. There is something more special going on at those peaks (related to the quarks).
unscientific said:
Peak at 100GeV comes from production of top quarks.
Compare that to the mass of two top quarks. Can that be right?
 
mfb said:
Not all of them are possible over the full range of 2 to 20 GeV.
Not the general production, that leads to the flat R you calculated. There is something more special going on at those peaks (related to the quarks).
Compare that to the mass of two top quarks. Can that be right?

Mass of quarks d,u,s,c,b are given by 0.005, 0.003, 0.1, 1.2, 4.2 GeV respectively. That's clearly lower than 20GeV, what is restricting their formation?

If it's not the heavier quarks that's forming, I'm guessing it's the formation of hadrons?

You're right in saying that two top quarks will have energy of 340GeV, but can't a combination of top and other quarks be formed?
 
At 20 GeV all of them are possible, but at 2 GeV that is not true.
unscientific said:
If it's not the heavier quarks that's forming, I'm guessing it's the formation of hadrons?
There is a different particle at 90 GeV.

The top quark decays before it hadronizes, and even if it would form hadrons they would be above the top mass. Hadrons do not have an energy significantly above the quark masses - of the order of 1 GeV more is possible, but not 80 GeV.
 
mfb said:
At 20 GeV all of them are possible, but at 2 GeV that is not true.
There is a different particle at 90 GeV.

The top quark decays before it hadronizes, and even if it would form hadrons they would be above the top mass. Hadrons do not have an energy significantly above the quark masses - of the order of 1 GeV more is possible, but not 80 GeV.

Sorry I should have been more specific. Here are the range for quark production:

uds : 2-3 GeV
udsc: 3-10 GeV
udscb: 10-20 GeV

quarkproduction2.png
To summarize, peak at 3GeV corresponds to the J/psi ##(c \bar c)## meson being produced, peak at 10GeV corresponds to the upsilon ##(b \bar b)## meson being produced and peak at 90 GeV corresponds to the ##Z^0## Boson.

But Z meson is produced by coupling to all the standard model fermions.

zboson.png


Hadronic: ##f = u, d, s ... ##
Leptonic: ## f = e^-, \mu^-, \tau^-##
Other (invis): ##f = \nu_{e, \mu, \tau}##

None of these have mass 45 GeV. How does the Z boson get its mass of 90 GeV?
 
Last edited:
Right.

unscientific said:
None of these have mass 45 GeV. How does the Z boson get its mass of 90 GeV?
It is an elementary particle with this mass. It is not a bound state of other particles.
 
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