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All baryons must have all three colors present, ''r, g, ''and'' b'', and so are colorless, and exhibit no external evidence of the strong color interaction. Likewise, regardless of the flavor combinations in a meson, the colors of the quark-antiquark cancel, so the meson also is colorless to the outside world.<ref name=McParland/>
All baryons must have all three colors present, ''r, g, ''and'' b'', and so are colorless, and exhibit no external evidence of the strong color interaction. Likewise, regardless of the flavor combinations in a meson, the colors of the quark-antiquark cancel, so the meson also is colorless to the outside world.<ref name=McParland/> The role of the color force is thus simply to hold the quark combinations together, which is accomplished by exchange of gluons among the constituent quarks.


===Quanta===
===Quanta===

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The fundamental particles and messenger quanta of the Standard Model.

The Standard Model of particle physics is the mathematical theory that describes the weak, electromagnetic and strong interactions between leptons and quarks, the basic particles of particle physics. This model is very strongly supported by experimental observations, and is considered to be a major achievement (perhaps the most outstanding achievement) of theoretical physics. It does not, however, treat the gravitational force, inclusion of which remains an elusive goal of the ultimate "theory of everything". The Standard Model is accordingly not consistent with general relativity. The theory is consistent with special relativity.

The model is described only qualitatively in this article, and neither mathematical details nor experimental phenomenology are provided. The objective here is only an introduction to the basic terminology for particles in the Standard Model and their interactions.

Particles and interactions

Various decay reactions and high-energy interactions between the multitudes of sub-atomic particles (initially just neutrons, protons, electrons, and photons, but extended to observations of pions, kaons, J/ψ's or jay-psi’s, upsilons, and so forth)[1] are well known experimentally, and transcend the Standard Model. The Standard Model explains these observations through the introduction of fundamental particles: spin 1/2 fermions of two types: leptons and quarks and the forces between them. Fundamental particle interactions are viewed as exchange forces, which is to say the trading back and forth of force carriers, which are different kinds of particle that represent quanta of the underlying force fields. So, for example, the quanta of the electromagnetic field are photons. The strength of an electromagnetic field is dictated by the number of photons that make it up, and the exchange of photons between particles with electric charge is the mechanism underlying the field's ability to exert an electromagnetic force upon these bodies.

Leptons

Leptons are one type of fundamental particle. They have spin 1/2 and are not subject to the strong force. The known leptons are said to be of three families or generations (labeled in the table as 1, 2, 3) and of six flavors, a generic term for the particle names. They are listed in the table below. Their antiparticles also are leptons with opposite electric charge Q and opposite Lepton number Le,μ,τ. For example, the anti-electron or positron has a positive electric charge and a negative electron lepton number Le=−1.

Lepton flavor properties
Particle name Symbol Family/Generation Q (e) Le Lμ Lτ Mass (MeV) Lifetime (s)
Electron e 1 −1 +1 0 0 0.510 998 928(11)[2] Stable
Muon μ 2 −1 0 +1 0 105.658 3715(35)[3] 2.197019(21) × 10−6
Tau τ 3 −1 0 0 +1 1776.82(16)[4] 2.906(10) × 10-13
Electron neutrino νe 1 0 +1 0 0 < 225 × 10−6 [5] Unknown
Muon neutrino νμ 2 0 0 +1 0 < 0.19 [5] Unknown
Tau neutrino ντ 3 0 0 0 +1 < 18.2 [5] Unknown

Quarks

Quarks are a type of particle with spin 1/2 that are subject to strong, weak and electromagnetic forces. The known quarks are listed in the table below. The kinds of quark (u, d, c, s, t, d) are referred to as the flavor index of the quark, and besides a flavor index, each quark has a color index, which may be any of three colors: red, green and blue (r, g, b). In a stretched analogy to light, a combination of three quarks with all three colors is referred to as "white" or "colorless" and exhibits no external evidence of a color index. Their antiparticles also are quarks, but carry anti-colors: anti-red, anti-green, anti-blue. A combination of quark and anti-quark with a color and its anti-color is "white" or "colorless".

Unlike a particle's electric charge, which can be any multiple of the elementary charge e, a quark can carry only one unit of color. The elementary unit of color has not been measured, a result of failure to observe an isolated quark.

Quark flavor properties
Name Symbol Family/Generation B Q(e) I3 C S T B′ Mass (MeV) Antiparticle Antiparticle symbol
Up u 1 +1/3 +2/3 +1/2 0 0 0 0 2.34 ± 0.19 [6] Antiup ū
Down d 1 +1/3 −1/3 −1/2 0 0 0 0 4.78 ± 0.11 [6] Antidown
Charm c 2 +1/3 +2/3 0 +1 0 0 0 1.294 ± 0.004 × 103 [6] Anticharm
Strange s 2 +1/3 −1/3 0 0 −1 0 0 100.2 ± 2.4[6] Antistrange
Top t 3 +1/3 +2/3 0 0 0 +1 0 172.9 ±0.6 ±0.9 × 103 [6] Antitop
Bottom b 3 +1/3 −1/3 0 0 0 0 −1 4.19 (+0.18) (−0.06) × 103 [6] Antibottom
B = baryon number, Q = electric charge, I3 = isospin, C = charm, S = strangeness, T = topness, B′ = bottomness.
* Notation such as ±xxx denotes measurement uncertainty. In the case of the top quark, the first uncertainty is statistical in nature, and the second is systematic.

The quarks carry fractional electric charge. However, no quark has been observed in isolation, so a "free" fractional electric charge has not been seen.

The quark structure of some sub-atomic particles is shown in the following tables.[7]

Some baryons
Name Symbol Quark structure Electric charge Spin
Proton +1 1/2
Antiproton −1 1/2
Neutron 0 1/2
Lambda 0 1/2
Omega −1 3/2

Some mesons
Name Symbol Quark structure Electric charge Spin
Pion +1 0
Kaon −1 0
Rho +1 1
D-plus +1 0
Eta-c 0 0

All baryons must have all three colors present, r, g, and b, and so are colorless, and exhibit no external evidence of the strong color interaction. Likewise, regardless of the flavor combinations in a meson, the colors of the quark-antiquark cancel, so the meson also is colorless to the outside world.[8] The role of the color force is thus simply to hold the quark combinations together, which is accomplished by exchange of gluons among the constituent quarks.

Quanta

Because gravitation is not included in the standard model, there are three type of interaction included. Each type of interaction is mediated by exchange of quanta that are bosons, sometimes called messenger particles.[9]

Messenger particles
Interaction field Particle name Symbol Spin Range (m) Mass(GeV)
Electromagnetic field Photon γ 1 < 10−27 [10]
Weak field Weak bosons W+, W, Z 1 ≈ 10−17 MW=80.399±0.023;[11] MZ=91.1876±0.0021[12]
Strong field Gluons (8) g 1 ≈ 10−15 0[13]

Photons

The photon mediates the electromagnetic force and has a very long history. It has neither electric charge nor mass.

Weak gauge bosons

The massive W+, W, Z, weak bosons are the messenger particles for the weak force. Their nonzero mass is expected from the Standard Model because of the introduction of the Higgs boson, a particle yet to be seen experimentally, and conjectured to have a mass as large as 1000 GeV.[14] The W+, W are antiparticles of each other and the Z boson is its own antiparticle.

Gluons

Gluons mediate the strong force as an exchange force due to color, one property of quarks. A gluon carries both a color and an anti-color. When a quark emits a gluon, its color changes in a way dependent upon the color/anti-color of the emitted gluon. For example, a red quark can emit a red-antiblue gluon, becoming a blue quark. There are nine possible color-anticolor combinations of r, g, b, which leads to only eight possible gluons because emission by a quark of one color-anticolor combination doesn't change the state of a quark and cannot act as a messenger.[15] The remaining eight gluon color combinations are shown below.[14]

Gluon color combinations

The peculiar combinations: , ,    result from arranging all the possible combinations of colors and anti-colors as symmetrized unit vectors in a space of color/anti-color products.

Nuclear forces and mesons

(PD) Image: John R. Brews
A neutron and proton trade identities by exchange of a π in the Yukawa model.

In 1935 Yukawa invented the meson theory for explaining the nuclear forces holding atomic nucleii together, an assemblage of neutrons and protons. The mesons were postulated to exist in three forms: π+, π0, and π , all of spin zero, today called pions.[16] The behavior of nuclear forces was explained as an exchange of pions.[17] An example is shown in the figure, where the neutron (lower right) emits a pion of negative electric charge to become a positive proton (upper right), while the proton (lower left) absorbs the pion to become a neutron (upper left).[18]

Incidental experimental observation of the muon or μ-meson in 1936 appeared to provide the π meson needed by the theory, but soon it was found that the muon did not interact with the nucleus and had spin 1/2 (it is a lepton). Later, in 1947, the actual π-meson or pion was discovered, and the pion did interact with the nucleus. Today all three pions have been observed, π+0, and π, the last observed being the neutral pion found in 1950.

A more refined theory of nuclear interactions is based upon the Standard Model. Today, pions are considered to be quark-antiquark pairs. The π is a d-quark combined with a ū-antiquark, and a π+ is the other way around, making each the antiparticle of the other. The π0 is a u-quark combined with a ū-antiquark, and therefore its own antiparticle. Because the pions are colorless (the anti-quark in a pion always has the anti-color to the quark, regardless of its flavor), their exchange between nucleons is not a simple color exchange, but a residual color force sometimes referred to as a color van der Waals force, an analogy to the weak electromagnetic attraction between electric charge-neutral atomic complexes.[19] In any event, nuclear forces are not considered fundamental today, but are a consequence of the underlying strong forces between quarks, also called chromodynamic forces or color forces. On that basis, nuclear forces are fundamentally based upon color, and only approximated by the Yukawa theory.

References

  1. For an introduction, see Lincoln Wolfenstein, Joao P. Silva (2010). “Chapter 5: The birth of particle physics”, Exploring Fundamental Particles. Taylor & Francis, pp. 47 ff. ISBN 1439836124. 
  2. Electron mass energy equivalent in MeV mec02. NIST. Retrieved on 2011-08-26.
  3. Muon mass energy equivalent in MeV mμc02. NIST. Retrieved on 2011-08-26.
  4. Tau mass energy equivalent in MeV mτc02. NIST. Retrieved on 2011-08-26.
  5. 5.0 5.1 5.2 K. Nakamura et al. (June 16, 2011). Neutrino properties. PDG Particle listings. Particle Data Group.
  6. 6.0 6.1 6.2 6.3 6.4 6.5 K. Nakamura et al. (January 15, 2011). QUARKS. PDG Particle listings. Particle Data Group.
  7. Information for tables from Tai L. Chow (2008). “Tables 9.3 and 9.4”, Gravity, black holes, and the very early universe: an introduction to general relativity and cosmology. Springer, p. 168. ISBN 0387736298. 
  8. Brian J. McParland (2010). Nuclear Medicine Radiation Dosimetry: Advanced Theoretical Principles. Springer, p. 36. ISBN 1848821255. 
  9. Britannica Educational Publishing (2011). “The basic forces and their messenger particles”, Erik Gregersen, ed: The Britannica Guide to Particle Physics. The Rosen Publishing Group, p. 15. ISBN 1615303820. 
  10. K. Nakamura et al. (June 16, 2011). γ. PDG Particle listings. Particle Data Group.
  11. K. Nakamura et al. (June 16, 2011). W. PDG Particle listings. Particle Data Group.
  12. K. Nakamura et al. (June 16, 2011). Z. PDG Particle listings. Particle Data Group.
  13. K. Nakamura et al. (June 16, 2011). g or gluon. PDG Particle listings. Particle Data Group.
  14. 14.0 14.1 Andrew Watson (2004). “Table 4.4: The eight gluon color configurations”, The quantum quark. Cambridge University Press, p. 175. ISBN 0521829070. 
  15. O. M. Boyarkin, Alfred L. Heinzerton (2007). Introduction to Physics of Elementary Particles. Nova Publishers, p. 2. ISBN 160021200X. 
  16. The properties of the pions from a modern standpoint are described in Yorikiyo Nagashima (2010). “§13.2 Pions”, Elementary Particle Physics: Volume 1: Quantum Field Theory and Particles. Wiley-VCH, p. 449. ISBN 3527409629. 
  17. For an historical outline, see for example Burton Feldman (2001). The Nobel Prize: A History of Genius, Controversy, and Prestige. Arcade Publishing, p. 169. ISBN 1559705922. 
  18. The corresponding diagram using quarks is found in Charis Anastopoulos (2008). “Figure 8.5: Quarks and strong interactions”, Particle or wave: the evolution of the concept of matter in modern physics. Princeton University Press, p. 299. ISBN 0691135126. 
  19. Raymond A. Serway, Chris Vuille (2006). Essentials of college physics. Cengage Learning/Brooks Cole, p. 772. ISBN 0495106194.