List of particles

This article includes a list of the different types of atomic- and sub-atomic particles found or believed to exist in the whole of the universe. For individual lists of the different particles, see the list below.

Elementary particles

Elementary particles are particles with no measurable internal structure; that is, they are not composed of other particles. They are the fundamental objects of quantum field theory. Many families and sub-families of elementary particles exist. Elementary particles are classified according to their spin. Fermions have half-integer spin while bosons have integer spin. All the particles of the Standard Model have been experimentally observed, recently including the Higgs boson.[1][2]

Fermions

Fermions are one of the two fundamental classes of particles, the other being bosons. Fermion particles are described by Fermi–Dirac statistics and have quantum numbers described by the Pauli exclusion principle. They include the quarks and leptons, as well as any composite particles consisting of an odd number of these, such as all baryons and many atoms and nuclei.

Fermions have half-integer spin; for all known elementary fermions this is 12. All known fermions, except neutrinos, are also Dirac fermions; that is, each known fermion has its own distinct antiparticle. It is not known whether the neutrino is a Dirac fermion or a Majorana fermion.[3] Fermions are the basic building blocks of all matter. They are classified according to whether they interact via the color force or not. In the Standard Model, there are 12 types of elementary fermions: six quarks and six leptons.

Quarks

Quarks are the fundamental constituents of hadrons and interact via the strong interaction. Quarks are the only known carriers of fractional charge, but because they combine in groups of three (baryons) or in pairs of one quark and one antiquark (mesons), only integer charge is observed in nature. Their respective antiparticles are the antiquarks, which are identical except that they carry the opposite electric charge (for example the up quark carries charge +23, while the up antiquark carries charge −23), color charge, and baryon number. There are six flavors of quarks; the three positively charged quarks are called "up-type quarks" and the three negatively charged quarks are called "down-type quarks".

Quarks
Name Symbol Antiparticle Charge
(e)
Mass (MeV/c2) [4] Spin
up u
u
+23 2.2+0.6
0.4
½
down d
d
13 4.6+0.5
0.4
½
charm c
c
+23 1280±30 ½
strange s
s
13 96+8
4
½
top t
t
+23 173,100±600 ½
bottom b
b
13 4,180+40
30
½

Leptons

Leptons do not interact via the strong interaction. Their respective antiparticles are the antileptons which are identical, except for the fact that they carry the opposite electric charge and lepton number. The antiparticle of an electron is an antielectron, which is nearly always called a "positron" for historical reasons. There are six leptons in total; the three charged leptons are called "electron-like leptons", while the neutral leptons are called "neutrinos". Neutrinos are known to oscillate, so that neutrinos of definite flavor do not have definite mass, rather they exist in a superposition of mass eigenstates. The hypothetical heavy right-handed neutrino, called a "sterile neutrino", has been left off the list.

Leptons
Name Symbol Antiparticle Charge
(e)
Mass (MeV/c2) [4]
Electron
e

e+
−1 0.511[note 1]
Electron neutrino
ν
e

ν
e
0 < 0.0000022
Muon
μ

μ+
−1 105.7[note 2]
Muon neutrino
ν
μ

ν
μ
0 < 0.170
Tau
τ

τ+
−1 1,776.86±0.12
Tau neutrino
ν
τ

ν
τ
0 < 15.5
  1. The electron mass is known very precisely as 0.5109989461±0.0000000031 MeV
  2. The muon mass known very precisely as 105.6583745±0.0000024 MeV

Bosons

Bosons are one of the two fundamental classes of particles, the other being fermions. Bosons are characterized by Bose–Einstein statistics and all have integer spins. Bosons may be either elementary, like photons and gluons, or composite, like mesons.

According to the Standard Model the elementary bosons are:

Name Symbol Antiparticle Charge (e) Spin Mass (GeV/c2) [4] Interaction mediated Existence
Photon γ Self 0 1 0 Electromagnetism Confirmed
W boson
W

W+
−1 1 80.385±0.015 Weak interaction Confirmed
Z boson
Z
Self 0 1 91.1875±0.0021 Weak interaction Confirmed
Gluon
g
Self 0 1 0 Strong interaction Confirmed
Higgs boson
H0
Self 0 0 125.09±0.24 Mass Confirmed
Graviton G Self 0 2 0 Gravitation Unconfirmed

Elementary bosons responsible for the four fundamental forces of nature are called force particles (gauge bosons). Strong interaction is mediated by the gluon, weak interaction is mediated by the W and Z bosons, and it is sometimes hypothetized that gravitation is mediated by the graviton, although it is not predicted by the Standard Model but by other theories in the framework of quantum field theory.

The Higgs boson is postulated by the electroweak theory primarily to explain the origin of particle masses. In a process known as the "Higgs mechanism", the Higgs boson and the other gauge bosons in the Standard Model acquire mass via spontaneous symmetry breaking of the SU(2) gauge symmetry. The Minimal Supersymmetric Standard Model (MSSM) predicts several Higgs bosons. A new particle expected to be the Higgs boson was observed at the CERN/LHC on March 14, 2013, around the energy of 126.5 GeV with an accuracy of close to five sigma (99.9999%, which is accepted as definitive). The Higgs mechanism giving mass to other particles has not been observed yet.

Hypothetical particles

Supersymmetric theories predict the existence of more particles, none of which have been confirmed experimentally as of 2016:

Superpartners (Sparticles)
Superpartner Superpartner of Spin Notes
neutralino neutral bosons 12 The neutralinos are superpositions of the superpartners of neutral Standard Model bosons: neutral Higgs boson, Z boson and photon.
The lightest neutralino is a leading candidate for dark matter.
The MSSM predicts four neutralinos.
chargino charged bosons 12 The charginos are superpositions of the superpartners of charged Standard Model bosons: charged Higgs boson and W boson.
The MSSM predicts two pairs of charginos.
photino photon 12 Mixing with zino and neutral Higgsinos for neutralinos.
wino, zino W± and Z0 bosons 12 The charged wino mixing with the charged Higgsino for charginos, for the zino see line above.
Higgsino Higgs boson 0 For supersymmetry there is a need for several Higgs bosons, neutral and charged, according with their superpartners.
gluino gluon 12 Eight gluons and eight gluinos.
gravitino graviton 32 Predicted by supergravity (SUGRA). The graviton is hypothetical, too – see next table.
sleptons leptons 0 The superpartners of the leptons (electron, muon, tau) and the neutrinos.
sneutrino neutrino 0 Introduced by many extensions of the Standard Supermodel, and may be needed to explain the LSND results.
A special role has the sterile sneutrino, the supersymmetric counterpart of the hypothetical right-handed neutrino, called the "sterile neutrino".
squarks quarks 0 The stop squark (superpartner of the top quark) is thought to have a low mass and is often the subject of experimental searches.

Note: just as the photon, Z boson and W± bosons are superpositions of the B0, W0, W1, and W2 fields – the photino, zino, and wino± are superpositions of the bino0, wino0, wino1, and wino2 by definition.
No matter if one uses the original gauginos or this superpositions as a basis, the only predicted physical particles are neutralinos and charginos as a superposition of them together with the Higgsinos.

Other theories predict the existence of additional bosons:

Other hypothetical bosons and fermions
Name Spin Notes
graviton 2 Has been proposed to mediate gravity in theories of quantum gravity.
dual graviton 2 Has been hypothesized as dual of graviton under electric-magnetic duality in supergravity.
graviscalar 0 Also known as "radion".
graviphoton 1 Also known as "gravivector".[5]
axion 0 A pseudoscalar particle introduced in Peccei–Quinn theory to solve the strong-CP problem.
axino 12 Superpartner of the axion. Forms, together with the saxion and axion, a supermultiplet in supersymmetric extensions of Peccei–Quinn theory.
saxion 0
branon ? Predicted in brane world models.
dilaton 0 Predicted in some string theories.
dilatino 12 Superpartner of the dilaton.
X and Y bosons 1 These leptoquarks are predicted by GUT theories to be heavier equivalents of the W and Z.
W' and Z' bosons 1
magnetic photon ? A. Salam (1966). "Magnetic monopole and two photon theories of C-violation." Physics Letters 22 (5): 683–684.
majoron 0 Predicted to understand neutrino masses by the seesaw mechanism.
majorana fermion 12 ; 32 ?... gluino, neutralino, or other – is its own antiparticle.
chameleon 0 a possible candidate for dark energy and dark matter, and may contribute to cosmic inflation.

Mirror particles are predicted by theories that restore parity symmetry.

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

"Tachyon" is a generic name for hypothetical particles that travel faster than the speed of light (and so paradoxically experience time in reverse due to inversal of Theory of relativity) and have an imaginary rest mass.

Preons were suggested as subparticles of quarks and leptons, but modern collider experiments have all but ruled out their existence.

Kaluza–Klein towers of particles are predicted by some models of extra dimensions. The extra-dimensional momentum is manifested as extra mass in four-dimensional spacetime.

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

A combination of three u, d or s-quarks with a total spin of 32 form the so-called "baryon decuplet".
Proton quark structure: 2 up quarks and 1 down quark. The gluon tubes or flux tubes are now known to be Y shaped.

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

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

Mesons

Mesons of spin 0 form a nonet

Ordinary mesons are made up of a valence quark and a valence antiquark. Because mesons have spin of 0 or 1 and are not themselves elementary particles, they are "composite" bosons. Examples of mesons include the pion, kaon, and the J/ψ. In quantum hydrodynamic models, mesons mediate the residual strong force between nucleons.

At one time or another, positive signatures have been reported for all of the following exotic mesons but their existences have yet to be confirmed.

Atomic nuclei

A semi-accurate depiction of the helium atom. In the nucleus, the protons are in red and neutrons are in purple. In reality, the nucleus is also spherically symmetrical.

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 table of nuclides for a complete 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. To date, 118 elements have been discovered or created.

The atomic nucleus consists of protons and neutrons. Protons and neutrons are, in turn, made of quarks.

Molecules

Molecules are the smallest particles into which a non-elemental substance can be divided while maintaining the physical properties of the substance. Each type of molecule corresponds to a specific chemical compound. Molecules are a composite of two or more atoms. See list of compounds for a list of molecules. A molecule is generally combined in a fixed proportion. It is the most basic unit of matter and is homogenous.

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 are a selection of field excitations, called quasi-particles, that can be created and explored. These include:

Other

Classification by speed

See also

References

  1. Khachatryan, V.; et al. (CMS Collaboration) (2012). "Observation of a new boson at a mass of 125 GeV with the CMS experiment at the LHC". Physics Letters B. 716 (2012): 30. Bibcode:2012PhLB..716...30C. arXiv:1207.7235Freely accessible. doi:10.1016/j.physletb.2012.08.021.
  2. Abajyan, T.; et al. (ATLAS Collaboration) (2012). "Observation of a new particle in the search for the Standard Model Higgs boson with the ATLAS detector at the LHC". Physics Letters B. 716 (2012): 1–29. Bibcode:2012PhLB..716....1A. arXiv:1207.7214Freely accessible. doi:10.1016/j.physletb.2012.08.020.
  3. Kayser, Boris (2010). "Two Questions About Neutrinos". arXiv:1012.4469Freely accessible [hep-ph].
  4. 1 2 3 Particle Data Group (2016). "Review of Particle Physics". Chinese Physics C. 40: 100001.
  5. Maartens, R. (2004). "Brane-World Gravity" (PDF). Living Reviews in Relativity. 7: 7. Bibcode:2004LRR.....7....7M. arXiv:gr-qc/0312059Freely accessible. doi:10.12942/lrr-2004-7.
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