- Also called:
- elementary particle
- Related Topics:
- quark
- CP violation
- symmetry
- quantum field theory
- Higgs boson
Since the 1930s physicists have been aware of a force within the atomic nucleus that is responsible for certain types of radioactivity that are classed together as beta decay. A typical example of beta decay occurs when a neutron transmutes into a proton. The force that underlies this process is known as the weak force to distinguish it from the strong force that binds quarks together (see below The strong force).
The correct gauge field theory for the weak force incorporates the quantum field theory of electromagnetism (quantum electrodynamics) and is called electroweak theory. It treats the weak force and the electromagnetic force on an equal footing by regarding them as different manifestations of a more-fundamental electroweak force, rather as electricity and magnetism appear as different aspects of the electromagnetic force.
The electroweak theory requires four gauge bosons. One of these is the photon of electromagnetism; the other three are involved in reactions that occur via the weak force. These weak gauge bosons include two electrically charged versions, called W+ and W−, where the signs indicate the charge, and a neutral variety called Z0, where the zero indicates no charge. Like the photon, the W and Z particles have a spin quantum number of 1; unlike the photon, they are very massive. The W particles have a mass of about 80.4 GeV, while the mass of the Z0 particle is 91.187 GeV. By comparison, the mass of the proton is 0.94 GeV, or about one-hundredth that of the Z particle. (Strictly speaking, mass should be given in units of energy/c2, where c is the velocity of light. However, common practice is to set c = 1 so that mass is quoted simply in units of energy, eV, as in this paragraph.)
The charged W particles are responsible for processes, such as beta decay, in which the charge of the participating particles changes hands. For example, when a neutron transmutes into a proton, it emits a W−; thus, the overall charge remains zero before and after the decay process. The W particle involved in this process is a virtual particle. Because its mass is far greater than that of the neutron, the only way that it can be emitted by the lightweight neutron is for its existence to be fleetingly short, within the requirements of the uncertainty principle. Indeed, the W− immediately transforms into an electron and an antineutrino, the particles that are observed in the laboratory as the products of neutron beta decay. Z particles are exchanged in similar reactions that involve no change in charge.
In the everyday world the weak force is weaker than the electromagnetic force but stronger than the gravitational force. Its range, however, is very short. Because of the large amounts of energy needed to create the large masses of the W and Z particles, the uncertainty principle ensures that a weak gauge boson cannot be borrowed for long, which limits the range of the force to distances less than 10−17 metre. The weak force between two protons in a nucleus is only 10−7 the strength of the electromagnetic force. As the electroweak theory reveals and as experiments confirm, however, this weak force becomes effectively stronger as the energies of the participating particles increase. When the energies reach 100 GeV or so—roughly the energy equivalent to the mass of the W and Z particles—the strength of the weak force becomes comparable to that of the electromagnetic force. This means that reactions that involve the exchange of a Z0 become as common as those in which a photon is exchanged. Moreover, at these energies real W and Z particles, as opposed to virtual ones, can be created in reactions.
Unlike the photon, which is stable and can in principle live forever, the heavy weak gauge bosons decay to lighter particles within an extremely brief lifetime of about 10−25 second. This is roughly a million million times shorter than experiments can measure directly, but physicists can detect the particles into which the W and Z particles decay and can thus infer their existence. (See the .)
The strong force
Although the aptly named strong force is the strongest of all the fundamental interactions, it, like the weak force, is short-ranged and is ineffective much beyond nuclear distances of 10−15 metre or so. Within the nucleus and, more specifically, within the protons and other particles that are built from quarks, however, the strong force rules supreme; between quarks in a proton, it can be almost 100 times stronger than the electromagnetic force, depending on the distance between the quarks.
During the 1970s physicists developed a theory for the strong force that is similar in structure to quantum electrodynamics. In this theory quarks are bound together within protons and neutrons by exchanging gauge bosons called gluons. The quarks carry a property called “colour” that is analogous to electric charge. Just as electrically charged particles experience the electromagnetic force and exchange photons, so colour-charged, or coloured, particles feel the strong force and exchange gluons. This property of colour gives rise in part to the name of the theory of the strong force: quantum chromodynamics.
Gluons are massless and have a spin quantum number of 1. In this respect they are much like photons, but they differ from photons in one crucial way. Whereas photons do not interact among themselves—because they are not electrically charged—gluons do carry colour charge. This means that gluons can interact together, which has an important effect in limiting the range of gluons and in confining quarks within protons and other particles.
There are three types of colour charge, called red, green, and blue, although there is no connection between the colour charge of quarks and gluons and colour in the usual sense. Quarks each carry a single colour charge, while gluons carry both a colour and an anticolour charge.
The strong force acts in such a way that quarks of different colour are attracted to one another; thus, red attracts green, blue attracts red, and so on. Quarks of the same colour, on the other hand, repel each other. The quarks can combine only in ways that give a net colour charge of zero. In particles that contain three quarks, such as protons, this is achieved by adding red, blue, and green. An alternative, observed in particles called mesons (see below Hadrons), is for a quark to couple with an antiquark of the same basic colour. In this case the colour of the quark and the anticolour of the antiquark cancel each other out. These combinations of three quarks (or three antiquarks) or of quark-antiquark pairs are the only combinations that the strong force seems to allow.
The constraint that only colourless objects can appear in nature seems to limit attempts to observe single quarks and free gluons. Although a quark can radiate a real gluon just as an electron can radiate a real photon, the gluon never emerges on its own into the surrounding environment. Instead, it somehow creates additional gluons, quarks, and antiquarks from its own energy and materializes as normal particles built from quarks. Similarly, it appears that the strong force keeps quarks permanently confined within larger particles. Attempts to knock quarks out of protons by, for example, knocking protons together at high energies succeed only in creating more particles—that is, in releasing new quarks and antiquarks that are bound together and are themselves confined by the strong force.
Classes of subatomic particles
From the early 1930s to the mid-1960s, studies of the composition of cosmic rays and experiments using particle accelerators revealed more than 200 types of subatomic particles. In order to comprehend this rich variety, physicists began to classify the particles according to their properties (such as mass, charge, and spin) and to their behaviour in response to the fundamental interactions—in particular, the weak and strong forces. The aim was to discover common features that would simplify the variety, much as the periodic table of chemical elements had done for the wealth of atoms discovered in the 19th century. An important result was that many of the particles, those classified as hadrons, were found to be composed of a much smaller number of more-elementary particles, the quarks. Today the quarks, together with the group of leptons, are recognized as fundamental particles of matter.
Leptons and antileptons
Leptons are a group of subatomic particles that do not experience the strong force. They do, however, feel the weak force and the gravitational force, and electrically charged leptons interact via the electromagnetic force. In essence, there are three types of electrically charged leptons and three types of neutral leptons, together with six related antileptons. In all three cases the charged lepton has a negative charge, whereas its antiparticle is positively charged. Physicists coined the name lepton from the Greek word for “slender” because, before the discovery of the tau in 1975, it seemed that the leptons were the lightest particles. Although the name is no longer appropriate, it has been retained to describe all spin-1/2 particles that do not feel the strong force.
