Nuclear force: Difference between revisions

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''See also the articles'' [[Quark]] ''and'' [[Standard Model]]
''See also the articles'' [[Quark]] ''and'' [[Standard Model]]


Today a more refined theory of nuclear interactions is based upon the [[Standard Model]]. In that model, pions are considered to be [[quark]]-antiquark pairs. The &pi;<sup>–</sup> is a ''d''-quark combined with a ''ū''-antiquark, and a &pi;<sup>+</sup> is the other way around, making each the antiparticle of the other. The &pi;<sup>0</sup> 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 forces|van der Waals force]]'', an analogy to the weak [[Maxwell equations|electromagnetic]] attraction between electric charge-neutral atomic complexes.<ref name=Serway/> 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.
Today a more refined theory of nuclear interactions is based upon the [[Standard Model]]. In that model, pions are considered to be [[quark]]-antiquark pairs. As indicated in the table above, the &pi;<sup>–</sup> is a ''d''-quark combined with a ''ū''-antiquark, and a &pi;<sup>+</sup> is the other way around, making each the antiparticle of the other. The &pi;<sup>0</sup> 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 forces|van der Waals force]]'', an analogy to the weak [[Maxwell equations|electromagnetic]] attraction between electric charge-neutral atomic complexes.<ref name=Serway/> 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==
==References==

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A neutron and proton trade identities by exchange of a π in the Yukawa model.

In physics, the nuclear force is the force holding assemblies of protons and neutrons together.

History

In 1935 Yukawa invented the meson theory for explaining the forces holding an assemblage of neutrons and protons together. The mesons were postulated to exist in three forms: π+, π0, and π , all of spin zero, today called pions.[1] The behavior of nuclear forces was explained as an exchange of pions.[2] 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).[3]

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 being the neutral pion found in 1950.

Pion properties

The main pion properties are tabulated below (overscores indicate antiparticles). Symbols u and d refer to the up-quark and the down-quark.

Pion properties
Symbol Quark structure Electric charge (units e) Spin Mass (MeV/c02) Lifetime (s) Main decay mode
[4] +1 0 139.5708 2.6033 × 10−8
[4] −1 0 139.5708 2.6033 × 10−8
[5] 0 0 134.9766 0.84 × 10−16

In the Standard Model the pions are colorless: the antiquark of the quark-antiquark pair must possess the anticolor of the quark.

Modern formulation

See also the articles Quark and Standard Model

Today a more refined theory of nuclear interactions is based upon the Standard Model. In that model, pions are considered to be quark-antiquark pairs. As indicated in the table above, 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.[6] 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. 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. 
  2. 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. 
  3. 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. 
  4. 4.0 4.1 K. Nakamura et al. ((2010) and 2011 partial update for the 2012 edition). π±. Particle Data Group. Retrieved on 2011-09-02.
  5. K. Nakamura et al. ((2010) and 2011 partial update for the 2012 edition). π0. Particle Data Group. Retrieved on 2011-09-02.
  6. Raymond A. Serway, Chris Vuille (2006). Essentials of college physics. Cengage Learning/Brooks Cole, p. 772. ISBN 0495106194.