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1.7 Quark Color
Much informative quark physics has been revealed in experiments with e+e- colliding beams. We mention here experiments in the range between centre of mass energies 10 GeV and the threshold energy, around 90 GeV, at which the Z boson can be produced.
Figure 1.6. The lowest order Feynman diagram (Chapter 8) for electromagnetic µ+µ- pair production in e+e- collisions. |
The e+e- annihilation cross-section (e+e- -> µ+µ-) is comparatively easy to measure, and is easy to calculate in the Weinberg-Salam electroweak theory, which we shall introduce in Chapter 12. At centre of mass energies much below 90 GeV the cross-section is dominated by the electromagnetic process represented by the Feynman diagram of Fig. 1.6. The muon pair are produced ``back-to-back'' in the centre of mass system, which for an e+e- collider is the laboratory system. To leading order in the fine-structure constant = e2 / (4 0 c), the differential cross-section for producing muons moving at an angle with respect to unpolarised incident beams is
where s is the square of the centre of mass energy (see Okun, 1982, p.
205). In the derivation of (1.1) the lepton masses are neglected.
Integrating with respect to ,
the total cross-section is
The quantity R (E) shown in Fig. 1.7 is
the ratio
At the lower energies many hadronic states are revealed as resonances,
but R seems to become approximately constant, R 4, at energies above
10 GeV up to about 40 GeV.
Figure 1.8. The lowest order Feynman
diagrams for quark-antiquark pair
production in e+e- collisions at energies below
the Z threshold.
As fundamental particles, quarks have the same electrodynamics as
muons, apart from the magnitude of their electric charge. The Feynman
diagrams which dominate the numerator of R in this range 10 GeV to 40
GeV are shown in Fig. 1.8. (The top quark has
a mass ~ 180 GeV and
will not contribute.) For each quark process the formula (1.2) holds,
except that e is replaced by the quark's electric charge at the quark
vertex, which suggests
This value is too low, by a factor of about 3.
In the Standard Model, the discrepancy is resolved by introducing
the idea of quark colour. A quark not only has a flavour index, u, d,
s, c, b, t, but also, for each flavour, a colour index. There are
postulated to be three basic states of colour, say red, green and blue
(r, g, b). With three quark colour states to each flavour, we have to
multiply the R of(1.4) by 3, to obtain
which is in excellent agreement with the data of
Fig. 1.7.
This invention of colour not only solves the problem of R but, most
significantly, solves the problem of the symmetry of the baryon
states. We have seen (Section 1.5) that in
the absence of any new
quantum number baryon states are completely symmetric in the
interchange of two quarks. However, if these state functions are
multiplied by an antisymmetric colour state function, the overall
state becomes antisymmetric, and the Pauli principle is preserved.
Strong support for the mechanism of quark production represented by
the Feynman diagrams of Fig. (1.8) is given by
other features in the
data from e+e- colliders. An
e+e- annihilation at high energies
produces many hadrons. These are mostly correlated into two
back-to-back jets. An example is shown in
Fig. 1.9. (The charged
particle tracks are curved because of the presence of an external
magnetic field: the curvature is related to the particle's momentum.)
The direction of a jet may be defined as the direction at the point of
production of the total momentum of all the hadrons associated with
it. The momenta of two back-to-back jets are equal and opposite. The
jet directions may be presumed to be the directions of the initial
quark-antiquark pair. This interpretation is corroborated by an
examination of the angular distribution of the jet directions of
two-jet events from many annihilations, with respect to the
e+e-
beams. The angular distribution is the same as that for muons
(equation (1.1)) after allowance has been made for the Z contribution,
which becomes significant as the energy for Z production is approached.
The hadron jets result from the original quark and antiquark
combining with quark-antiquark pairs generated from the vacuum. The
precise details of the processes involved are not yet fully
understood.