List of particles

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This is a list of particles in particle physics, including currently known and hypothetical elementary particles, as well as the composite particles that can be built up from them.

For a chronological listing of subatomic particles by discovery date, see Timeline of particle discoveries.

Image:Cloud chamber - visible trace of positron.JPG

Contents

Elementary particles

An elementary particle is a particle with no measurable internal structure, that is, it is not a composite of other particles. They are the fundamental objects of quantum field theory. Elementary particles can be classified according to their spin, with fermions having half-integer spin and bosons integer spin.

Standard Model

The Standard Model of particle physics is our current understanding of the physics of elementary particles. All Standard Model particles except the Higgs boson have been observed.

Fermions (half-integer spin)

Fermions have half-integer spin; for all known elementary fermions this is ½. Each fermion has its own distinct antiparticle. Fermions are the basic building blocks of all matter. They are classified according to whether they interact via the color force or not. According to the Standard Model, there are 12 flavors of elementary fermions: six quarks and six leptons.

Generation Name/Flavor Electric charge (e) Mass (MeV) Antiquark
1 Up (u) +2/3 1.5 to 4 antiup quark<math>(\overline{u})</math>
Down (d) −1/3 4 to 8 antidown quark <math>(\overline{d})</math>
2 Strange(s) −1/3 80 to 130 antistrange quark <math>(\overline{s})</math>
Charm(c) +2/3 1,150 to 1,350 anticharm quark <math>(\overline{c})</math>
3 Bottom(b) −1/3 4,100 to 4,400 antibottom quark <math>(\overline{b})</math>
Top(t) +2/3 178,000 ± 4,300 antitop quark<math>(\overline{t})</math>
  • Leptons do not interact via the color force. Their respective antiparticles are known as antileptons (although the antiparticle of the electron is called the positron for historical reasons). Leptons also exist in six flavors:
Charged lepton / antiparticle Neutrino / antineutrino
Name Symbol Electric charge (e) Mass (MeV) Name Symbol Electric charge (e) Mass (MeV)
Electron / Positron <math>e^- \, / \, e^+</math> −1 / +1 0.511 Electron neutrino / Electron antineutrino <math>\nu_e \, / \, \overline{\nu}_e</math> 0 < 0.000003
Muon <math>\mu^- \, / \, \mu^+ </math> −1 / +1 105.7 Muon neutrino / Muon antineutrino <math>\nu_\mu \, / \, \overline{\nu}_\mu</math> 0 < 0.19
Tau lepton <math>\tau^- \, / \, \tau^+</math> −1 / +1 1,777 Tau neutrino / Tau antineutrino <math>\nu_\tau \, / \, \overline{\nu}_\tau</math> 0 < 18.3

Note that the neutrino masses are known to be non-zero because of neutrino oscillation, but their masses are sufficiently light that they have not been measured directly as of 2006.

Bosons (integer spin)

Bosons have whole number spins. The fundamental forces of nature are mediated by gauge bosons, and mass is hypothesized to be created by the Higgs boson. According to the Standard Model the elementary bosons are:

Name Charge (e) Spin Mass (GeV) Force mediated
Photon 0 1 0 Electromagnetism
W± ±1 1 80.4 Weak nuclear
Z0 0 1 91.2 Weak nuclear
Gluon 0 1 0 Strong nuclear
Higgs 0 0 >112 See below

The Higgs boson (spin-0) is predicted by electroweak theory, and is the only Standard Model particle not yet observed. In the Higgs mechanism of the Standard Model, the massive Higgs boson is created by spontaneous symmetry breaking of the Higgs field. The intrinsic masses of the elementary particles (particularly the massive W± and Z0 bosons) would be explained by their interactions with this field. Many physicists expect the Higgs to be discovered at the Large Hadron Collider (LHC) particle accelerator now under construction at CERN.

Hypothetical particles

Supersymmetric theories predict the existence of more particles, none of which have been confirmed experimentally as of 2006.

Other theories predict the existence of additional bosons.

Magnetic monopole is a generic name for particles with non-zero magnetic charge. They are predicted by some GUT theories.

Composite particles

Hadrons

Hadrons are defined as strongly interacting composite particles. Hadrons are either:

Quark models, first proposed in 1964 independently by Murray Gell-Mann and George Zweig (who called quarks "aces"), describe the known hadrons as composed of valence quarks and/or antiquarks, tightly bound by the color force, which is mediated by gluons. A "sea" of virtual quark-antiquark pairs is also present in each hadron.

Baryons (fermions)

For a detailed list, see List of baryons.

Ordinary baryons (fermions) contain three valence quarks or three valence antiquarks each.

  • Nucleons are the fermionic constituents of normal atomic nuclei:
  • Hyperons such as the Λ, Σ, Ξ, and Ω particles, which contain one or more strange quarks, are short-lived and heavier than nucleons. They do not normally appear in atomic nuclei.
  • A number of charmed and bottom baryons have also been observed.

Some hints at the existence of exotic baryons have been found recently; however, negative results have also been reported. Their existence is uncertain.

  • Pentaquarks consist of four valence quarks and one valence antiquark.

Mesons (bosons)

For a detailed list, see List of mesons.

Ordinary mesons (bosons) contain a valence quark and a valence antiquark, and include the pion, kaon, the J/ψ, and many other types of mesons. In quantum hadrodynamic models, the strong force between nucleons is mediated by mesons.

Exotic mesons may also exist. Positive signatures have been reported for all of these particles at some time, but their existence is still somewhat uncertain.

  • Tetraquarks consist of two valence quarks and two valence antiquarks.
  • Glueballs are bound states of gluons with no valence quarks.
  • Hybrids consist of one or more valence quark-antiquark pairs and one or more real gluons.

Atomic nuclei

Atomic nuclei consist of protons and neutrons. Each type of nucleus contains a specific number of protons and a specific number of neutrons, and is called a nuclide or isotope. Nuclear reactions can change one nuclide into another. See Isotope table (complete) for a list of isotopes.

Atoms

Atoms are the smallest neutral particles into which matter can be divided by chemical reactions. An atom consists of a small, heavy nucleus surrounded by a relatively large, light cloud of electrons. Each type of atom corresponds to a specific chemical element, of which 111 have been officially named. Refer to the periodic table for an overview.

Molecules

Molecules are the smallest particles into which a substance can be divided while maintaining the physical properties of the substance. Each type of molecule corresponds to a specific chemical compound. Molecules are composites of one or more atoms. See list of compounds for a list of molecules.

Condensed matter

The field equations of condensed matter physics are remarkably similar to those of high energy particle physics. As a result, much of the theory of particle physics applies to condensed matter physics as well; in particular, there is a whole zoo of field excitations, called quasi-particles, that can be created and explored. These include:

Other

Categorisation by speed

  • A tardyon or bradyon travels slower than light and has a non-zero rest mass.
  • A luxon travels at the speed of light and has no rest mass.
  • A tachyon is a hypothetical particle that travels faster than the speed of light and has imaginary mass.

See also

References

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