Previous: Review of particle physics
Up: Introduction
Next: Simulation specifics
The flux tube model is a method for deciding which quarks are to interact by the exchange of gluon(s).
Quantum Chromo-Dynamics (QCD)
adds a new quantum number to quarks. This allows all three quarks
of a baryon to have otherwise similar quantum numbers. (The Pauli
exclusion principle would apply otherwise) Quarks therefore come in
three colours: red, green and blue. The combination of the three
colours in a baryon results in a colourless particle. QCD suggests
that the reason quarks are not observed in isolation is because only
colourless assemblies can be observed.
three-quark4Possible flux tube arrangements for three quarks
In the case of mesons, (pions, kaons, etc.) there are two quarks involved: a quark and an anti-quark. The anti-quark of a red quark is anti-red, so mesons are also colourless. (Similarly for blue and green quarks, but colour is degenerate in mesons)
Properly, the gluons that carry the strong force are also carriers of colour. This allows gluons to actually form complex arrangements not possible in quantum electrodynamics (QED). In the context of this experiment, an important aspect of the colour carrying nature of the gluons is that they can result in colour exchanges between the quarks. This mode of interaction has not been included.
In the flux tube model, the gluons become tubes connecting two
or three quarks. In a system of many quarks, the selection of which
pairs or triplets to connect is done in a way to minimize the total
distance involved. The longer the flux tube, the further that the
gluon particles are must travel. Since they travel at a finite
velocity, a longer distance requires a longer time. (See
figure )
two-quark-optimum5Optimal arrangement for three pairs
By the uncertainty equation,
, the longer
the virtual particle exists, the lower the energy available to be
borrowed to make the virtual particle.
mcr@ccs.carleton.ca