2 Families of quarks

All the quarks that appear in ordinary matter are either up or down quarks. However, in very high-energy situations, other quarks appear. The first "extra" quark discovered was called a strange quark; as higher-energy collisions became possible, the charm, bottom, and top quarks were discovered. These extra quarks seem to be merely higher-mass copies of ordinary quarks, just as the muon and the tauon are higher-mass copies of the electron.

One might wonder whether there are yet more families of quarks with even higher masses. Research at CERN has provided strong evidence that no such families exist. This experiment relied on accurate determination of the width in masses of the Z boson; by a subtle series of calculations, the numbers obtained could be shown to contradict the possibility that more families of quarks exist. See [1] for more information.

The number of families of quarks also affects the only other really high-energy situation we know of — the early Universe. The initial distribution of elements can be predicted using the Standard Model; any model with more heavy quarks would lead to a fraction of initial Helium-4 that is different from what is observed. Thus the number of quarks is confirmed by astronomical observations as well. See [2] for more information.

3 Color

According to the theory of quantum chromodynamics (QCD), quarks possess a property metaphorically called " color charge". Instead of just one charge type (with two signs, + and − in electromagnetism), color charge comes in 3 types. Quarks' colors are called "red", "green", or "blue" to suggest the primary colors, while anti-quarks are anti-red or "cyan", anti-green or "magenta", and anti-blue or "yellow". Due to confinement (described below), only color-neutral or "white" particles can exist separately: particles possessing color must be part of a "white" composite. Particles composed of one red, one green and one blue quark are called baryons; the proton and the neutron are the most important examples. Particles composed of a quark and an anti-quark of the corresponding anti-color are called mesons.

Particles of different color charge are attracted and particles of like color charge are repelled by the color force, which is transferred by gluons, particles that themselves carry color charge (one color and one anti-color). Therefore, colors of quarks are not static, but are constantly changed by gluons, though the composite hadron always remains neutral. In addition to holding quarks together in mesons and baryons, a residual effect of the color force, the strong nuclear force, holds the protons and neutrons together in the atomic nucleus.

Because the carriers of the strong force, the gluons, are themselves colored, the force between two quarks increases as the quarks are separated. Due to this mechanism, called confinement, quarks are almost never found free; they are always bound into color-neutral baryons or mesons. When we try to separate quarks, as happens in particle accelerator collisions, at some point it is more energetically favorable for a new quark/anti-quark pair to pop out of the vacuum than to allow the quarks to separate further. As a result of this, when quarks are produced in particle accelerators, instead of seeing the individual quarks in detectors, scientists see "jets" of many color-neutral particles (mesons and baryons), clustered together. This process is called hadronization or fragmentation, and is one of the least understood processes in particle physics. But if the pressure and temperature of the nucleonic reaction are high enough, a quark-gluon plasma forms, offering the first evidence of a free quark state.

4 History

The theory behind quarks was first suggested by physicists Murray Gell-Mann and George Zweig, who found they could explain apparent symmetries of the hadrons by considering them to belong to various groups, such as an octet of mesons called the "Eight-fold Way". The structure of these groups could be explained by postulating that the hadrons were composed of more fundamental particles belonging to an SU(3) triplet. In his 1964 paper (see below ) Gell-Mann notes:

A simpler and more elegant scheme can be constructed if we allow non-integral values of the charges. We then refer to the members u, d and s of the triplet as "quarks".

At the end of the paper, he cites James Joyce, Finnegans Wake ( 1939) p. 383, which contains the less-than-illuminating line "Three quarks for Muster Mark." Gell-Mann states elsewhere that "quark" was originally a nonsense word pronounced (sounding like "quart"), which he invented a few weeks before coming across the line from Finnegans Wake. At the same time, Zweig developed a similar scheme in which he called the new particles "aces"; however, this name failed to catch on.

5 See also

• Parton
• Rubik's Cube for an interesting parallel
• List of particles

6 External links

• Observation of the Top Quark at Fermilab
• A Positron Named Priscilla — A description of CERN's experiment to count the families of quarks
• Cosmological Models — A description of the Big Bang model, its predictions and problems.
• The original English word quark and its adaptation to particle physics
• A schematic model of baryons and mesons, Gell-Mann's 1964 paper

Particles in Physics - Elementary particles	[ }|action=edit}} Edit }]
Fermions : Quarks | Leptons
Gauge Bosons : Photon | W+, W- and Z0 bosons | Gluons
Not yet observed
Higgs boson | Graviton
Supersymmetric Partners : Neutralinos | Charginos | Gravitino | Gluinos | Squarks | Sleptons

Quark

<Hide>