Editing Strong interaction

{{Short description|Binding of quarks in subatomic particles}}
{{Redirect|Color force|the company|Color Force}}
[[File:Gluon_tube-color_confinement_animation.gif|thumb|upright=1.5|An animation of [[color confinement]], a property of the strong interaction. If energy is supplied to the quarks as shown, the [[gluon]] tube connecting [[Quark|quarks]] elongates until it reaches a point where it "snaps" and the energy added to the system results in the formation of a quark–[[antiquark]] pair. Thus single quarks are never seen in isolation.]]
[[File:Nuclear_Force_anim_smaller.gif|thumb|An animation of the strong interaction between a proton and a neutron, mediated by [[Pion|pions]]. The colored small double circles inside are [[gluon]]s.]]

In [[nuclear physics]] and [[particle physics]], the '''strong interaction''', also called the '''strong force''' or '''strong nuclear force''', is one of the four known [[fundamental interaction|fundamental interactions]]. It confines [[Quark|quarks]] into [[proton|protons]], [[neutron|neutrons]], and other [[hadron]] particles, and also binds neutrons and protons to create atomic nuclei, where it is called the [[nuclear force]].

Most of the [[mass–energy equivalence|mass]] of a [[proton]] or [[neutron]] is the result of the strong interaction energy; the individual quarks provide only about 1% of the mass of a proton. At the range of 10<sup>−15</sup>&nbsp;m (1 [[femtometer]], slightly more than the radius of a [[nucleon]]), the strong force is approximately 100 times as strong as [[electromagnetism]], 10<sup>6</sup> times as strong as the [[weak interaction]], and 10<sup>38</sup> times as strong as [[Gravity|gravitation]].<ref>Relative strength of interaction varies with distance. See for instance [[Matt Strassler]]'s essay, [http://profmattstrassler.com/articles-and-posts/particle-physics-basics/the-known-forces-of-nature/the-strength-of-the-known-forces/ "The strength of the known forces"].</ref>

In the context of atomic nuclei, the force binds protons and neutrons together to form a nucleus and is called the [[nuclear force]] (or ''residual strong force'').<ref name="auto"/> Because the force is mediated by massive, short lived [[mesons]] on this scale, the residual strong interaction obeys a distance-dependent behavior between nucleons that is quite different from when it is acting to bind quarks within hadrons. There are also differences in the [[binding energy|binding energies]] of the nuclear force with regard to [[nuclear fusion]] versus [[nuclear fission]]. Nuclear fusion accounts for most energy production in the [[Sun]] and other [[star]]s. Nuclear fission allows for decay of radioactive elements and [[isotope]]s, although it is often mediated by the weak interaction. Artificially, the energy associated with the nuclear force is partially released in [[nuclear power]] and [[nuclear weapons]], both in [[uranium]] or [[plutonium]]-based fission weapons and in fusion weapons like the [[hydrogen bomb]].<ref>{{cite web | archive-url=https://web.archive.org/web/20121218195010/https://netfiles.uiuc.edu/mragheb/www/NPRE%20402%20ME%20405%20Nuclear%20Power%20Engineering/Nuclear%20Processes%20The%20Strong%20Force.pdf | access-date=2023-10-03 | archive-date=2012-12-18 | title=Chapter 4 Nuclear Processes, The Strong Force | last=Ragheb | first=Magdi | publisher=University of Illinois | url= https://netfiles.uiuc.edu/mragheb/www/NPRE%20402%20ME%20405%20Nuclear%20Power%20Engineering/Nuclear%20Processes%20The%20Strong%20Force.pdf | url-status=dead}}</ref><ref>{{cite web | archive-url= https://web.archive.org/web/20230528145648/http://www.furryelephant.com/content/radioactivity/binding-energy-mass-defect/ | access-date=2023-10-03 | archive-date=2023-05-28 | title=Lesson 13: Binding energy and mass defect | author=<!--Not stated--> | website=Furry Elephant physics educational site | url= http://www.furryelephant.com/content/radioactivity/binding-energy-mass-defect/ | url-status=dead}}</ref>

== History ==
Before 1971, physicists were uncertain as to how the atomic nucleus was bound together. It was known that the nucleus was composed of [[proton]]s and [[neutron]]s and that protons possessed positive [[electric charge]], while neutrons were electrically neutral. By the understanding of physics at that time, positive charges would repel one another and the positively charged protons should cause the nucleus to fly apart. However, this was never observed. New physics was needed to explain this phenomenon.

A stronger attractive force was postulated to explain how the atomic nucleus was bound despite the protons' mutual [[electromagnetic repulsion]]. This hypothesized force was called the ''strong force'', which was believed to be a fundamental force that acted on the [[nucleons|protons and neutrons]] that make up the nucleus.

In 1964, [[Murray Gell-Mann]], and separately [[George Zweig]], proposed that [[baryon]]s, which include protons and neutrons, and [[meson]]s were composed of elementary particles. Zweig called the elementary particles "aces" while Gell-Mann called them "quarks"; the theory came to be called the [[quark model]].<ref>{{Cite journal |last=Wilczek |first=Frank |date=1982 |title=Quantum chromodynamics: The modern theory of the strong interaction |journal=Annual Review of Nuclear and Particle Science |volume=32 |issue=1 |pages=177–209 |doi=10.1146/annurev.ns.32.120182.001141|bibcode=1982ARNPS..32..177W }}</ref> The strong attraction between nucleons was the side-effect of a more fundamental force that bound the quarks together into protons and neutrons. The theory of [[quantum chromodynamics]] explains that quarks carry what is called a [[color charge]], although it has no relation to visible color.<ref>
{{cite book
 |last=Feynman |first=R.P. |author-link=Richard Feynman
 |year=1985
 |title=QED: The Strange Theory of Light and Matter
 |publisher=Princeton University Press
 |isbn=978-0-691-08388-9
 |page=136
 |quote=The idiot physicists, unable to come up with any wonderful Greek words anymore, call this type of polarization by the unfortunate name of 'color', which has nothing to do with color in the normal sense.
 |title-link=QED: The Strange Theory of Light and Matter
}}</ref> Quarks with unlike color charge attract one another as a result of the strong interaction, and the particle that mediates this was called the [[gluon]].

== Behavior of the strong interaction ==

The strong interaction is observable at two ranges, and mediated by different force carriers in each one. On a scale less than about 0.8&nbsp;[[femtometre|fm]] (roughly the radius of a nucleon), the force is carried by [[gluon|gluons]] and holds [[quark|quarks]] together to form protons, neutrons, and other hadrons. On a larger scale, up to about 3&nbsp;fm, the force is carried by [[meson|mesons]] and binds nucleons ([[proton|protons]] and [[neutron|neutrons]]) together to form the [[atomic nucleus|nucleus]] of an [[atom]].<ref name="auto">{{cite web| url = http://webhome.phy.duke.edu/~kolena/modern/forces.html#005| title = The four forces: the strong interaction Duke University Astrophysics Dept website}}</ref> In the former context, it is often known as the '''color force''', and is so strong that if hadrons are struck by high-energy particles, they produce [[Jet (particle physics)|jets]] of massive particles instead of emitting their constituents (quarks and gluons) as freely moving particles. This property of the strong force is called [[color confinement]].

{| class="wikitable" style="margin-left: auto; margin-right: auto; border: none;"
|+ Two layers of strong interaction
|-
! Interaction  !! range !! held !! carrier !! result
|-
| Strong || style=text-align:right |< {{val|0.8|u=fm}} || quark || gluon || hadron
|-
| Residual Strong || style=text-align:right | {{val|1|–|3|u=fm}}  || hadron || meson || nucleus
|}

=== Within hadrons ===
[[File:Gluon coupling.svg|thumb|right|400px|The fundamental [[coupling (physics)|couplings]] of the strong interaction, from left to right: (a) gluon radiation, (b) gluon splitting and (c,d) gluon self-coupling.]]
The word ''strong'' is used since the strong interaction is the "strongest" of the four fundamental forces. At a distance of 10<sup>−15</sup>&nbsp;m, its strength is around 100&nbsp;times that of the [[electromagnetic force]], some 10<sup>6</sup>&nbsp;times as great as that of the weak force, and about 10<sup>38</sup>&nbsp;times that of [[gravitation]].

The strong force is described by [[quantum chromodynamics]] (QCD), a part of the [[Standard Model]] of particle physics. Mathematically, QCD is a non-abelian [[gauge theory]] based on a local (gauge) [[symmetry group]] called [[SU(3)]].

The force carrier particle of the strong interaction is the gluon, a massless [[gauge boson]]. Gluons are thought to interact with quarks and other gluons by way of a type of charge called [[color charge]]. Color charge is analogous to electromagnetic charge, but it comes in three types (±red, ±green, and ±blue) rather than one, which results in different rules of behavior. These rules are described by [[quantum chromodynamics]] (QCD), the theory of quark–gluon interactions.
Unlike the [[photon]] in electromagnetism, which is neutral, the gluon carries a color charge. Quarks and gluons are the only fundamental particles that carry non-vanishing color charge, and hence they participate in strong interactions only with each other. The strong force is the expression of the gluon interaction with other quark and gluon particles.

All quarks and gluons in QCD interact with each other through the strong force. The strength of interaction is parameterized by the strong [[coupling constant]]. This strength is modified by the gauge color charge of the particle, a [[Group theory|group-theoretical]] property.

The strong force acts between quarks. Unlike all other forces (electromagnetic, weak, and gravitational), the strong force does not diminish in strength with increasing distance between pairs of quarks. After a limiting distance (about the size of a [[hadron]]) has been reached, it remains at a strength of about {{val|10000|ul=N}}, no matter how much farther the distance between the quarks.<ref name=Fritzsch1983/>{{rp|164}}  As the separation between the quarks grows, the energy added to the pair creates new pairs of matching quarks between the original two; hence it is impossible to isolate quarks. The explanation is that the amount of work done against a force of {{val|10000|u=N}} is enough to create particle–antiparticle pairs within a very short distance. The energy added to the system by pulling two quarks apart would create a pair of new quarks that will pair up with the original ones. In QCD, this phenomenon is called [[color confinement]]; as a result, only hadrons, not individual free quarks, can be observed. The failure of all experiments that have searched for [[free quark]]s is considered to be evidence of this phenomenon.

The elementary quark and gluon particles involved in a high energy collision are not directly observable. The interaction produces jets of newly created hadrons that are observable. Those hadrons are created, as a manifestation of mass–energy equivalence, when sufficient energy is deposited into a quark–quark bond, as when a quark in one proton is struck by a very fast quark of another impacting proton during a [[particle accelerator]] experiment. However, [[quark–gluon plasma]]s have been observed.<ref>{{cite news |url=http://physics.about.com/od/physicsqtot/fl/Quark-Gluon-Plasma.htm |title=Quark–gluon plasma is the most primordial state of matter |newspaper=About.com Education |access-date=2017-01-16 |archive-url=https://web.archive.org/web/20170118030724/http://physics.about.com/od/physicsqtot/fl/Quark-Gluon-Plasma.htm |archive-date=2017-01-18 |url-status=dead }}</ref>

=== Between hadrons ===
{{main|Nuclear force}}
[[File:Pn_Scatter_Quarks.svg|thumb|300x300px|A [[Feynman diagram]] (shown by the animation in the lead) with the individual [[quark]] constituents shown, to illustrate how the fundamental strong interaction gives rise to the [[nuclear force]]. Straight lines are quarks, while multi-colored loops are [[Gluon|gluons]] (the carriers of the fundamental force).]]
While color confinement implies that the strong force acts without distance-diminishment between pairs of quarks in compact collections of bound quarks (hadrons), at distances approaching or greater than the radius of a proton, a residual force (described below) remains. It manifests as a force between the "colorless" hadrons, and is known as the ''[[nuclear force]]'' or ''residual strong force'' (and historically as the ''strong nuclear force'').

The nuclear force acts between hadrons, known as [[meson]]s and [[baryon]]s. This "residual strong force", acting indirectly, transmits gluons that form part of the virtual [[pion|π]] and [[rho meson|ρ]]&nbsp;[[meson]]s, which, in turn, transmit the force between nucleons that holds the nucleus (beyond [[hydrogen-1]] nucleus) together.<ref>{{cite web |title=3. The Strong Force |url=http://www.damtp.cam.ac.uk/user/tong/pp/pp3.pdf |publisher=Department of Applied Mathematics and Theoretical Physics, University of Cambridge |access-date=10 January 2023 |archive-url=https://web.archive.org/web/20211022113145/http://www.damtp.cam.ac.uk/user/tong/pp/pp3.pdf |archive-date=22 October 2021}}</ref>

The residual strong force is thus a minor residuum of the strong force that binds quarks together into protons and neutrons. This same force is much weaker ''between'' neutrons and protons, because it is mostly neutralized ''within'' them, in the same way that electromagnetic forces between neutral atoms ([[van der Waals force]]s) are much weaker than the electromagnetic forces that hold electrons in association with the nucleus, forming the atoms.<ref name=Fritzsch1983>
{{cite book
 |last=Fritzsch |first=H.
 |year=1983
 |title=Quarks: The Stuff of Matter
 |url=https://archive.org/details/quarksstuffofmat00frit |url-access=registration |publisher=Basic Books
 |isbn=978-0-465-06781-7
 |pages=[https://archive.org/details/quarksstuffofmat00frit/page/167 167–168]
}}</ref>

Unlike the strong force, the residual strong force diminishes with distance, and does so rapidly. The decrease is approximately as a negative exponential power of distance, though there is no simple expression known for this; see ''[[Yukawa potential]]''. The rapid decrease with distance of the attractive residual force and the less rapid decrease of the repulsive electromagnetic force acting between protons within a nucleus, causes the instability of larger atomic nuclei, such as all those with [[atomic number]]s larger than 82 (the element lead).

Although the nuclear force is weaker than the strong interaction itself, it is still highly energetic: transitions produce [[gamma ray]]s. The mass of a nucleus is significantly different from the summed masses of the individual nucleons. This [[mass defect]] is due to the potential energy associated with the nuclear force. Differences between mass defects power [[nuclear fusion]] and [[nuclear fission]].

== Unification ==
The so-called [[Grand Unified Theory|Grand Unified Theories]] (GUT) aim to describe the strong interaction and the electroweak interaction as aspects of a single force, similarly to how the electromagnetic and weak interactions were unified by the Glashow–Weinberg–Salam model into [[electroweak interaction]]. The strong interaction has a property called [[asymptotic freedom]], wherein the strength of the strong force diminishes at higher energies (or temperatures). The theorized energy where its strength becomes equal to the electroweak interaction is the [[grand unification energy]]. However, no Grand Unified Theory has yet been successfully formulated to describe this process, and Grand Unification remains an [[List of unsolved problems in physics|unsolved problem in physics]].

If GUT is correct, after the [[Big Bang]] and during the [[electroweak epoch]] of the universe, the [[electroweak interaction|electroweak force]] separated from the strong force. Accordingly, a [[grand unification epoch]] is hypothesized to have existed prior to this.

== See also ==
{{portal|Physics}}
* [[Mathematical formulation of quantum mechanics]]
* [[Mathematical formulation of the Standard Model]]
* [[Nuclear binding energy]]
* [[QCD matter]]
* [[Quantum field theory]]
* [[Yukawa interaction]]

== References ==
{{reflist|30em}}

== Further reading ==
* {{cite web
 |last=Christman |first=J.R.
 |year=2001
 |title=MISN-0-280: ''The Strong Interaction''
 |url=https://physnet.org/modules/pdf_modules/m280.pdf
}}
* {{cite book
 |editor-last1=Ding |editor-first1=Minghui |editor-last2=Roberts |editor-first2=Craig |editor-last3=Schmidt |editor-first3=Sebastian
 |year=2024
 |title=Strong Interactions in the Standard Model: Massless Bosons to Compact Stars
 |publisher=[[MDPI]]
 |url=https://www.mdpi.com/books/reprint/9524-strong-interactions-in-the-standard-model-massless-bosons-to-compact-stars
 |isbn=978-3-7258-1502-9
}}
* {{Cite book
 |last1=Halzen
 |first1=F.
 |author-link1=Francis Halzen
 |last2=Martin
 |first2=A.D.
 |author-link2=Alan Martin (physicist)
 |year=1984
 |title=Quarks and Leptons: An Introductory Course in Modern Particle Physics
 |publisher=John Wiley & Sons
 |isbn=978-0-471-88741-6
 |url-access=registration
 |url=https://archive.org/details/quarksleptonsint0000halz
 }}
* {{cite book
 |last=Kane |first=G.L. |author-link=Gordon L. Kane
 |year=1987
 |title=Modern Elementary Particle Physics
 |publisher=Perseus Books
 |isbn=978-0-201-11749-3
}}
* {{cite book
 |last=Morris |first=R.
 |year=2003
 |title=The Last Sorcerers: The Path from Alchemy to the Periodic Table
 |url=https://archive.org/details/lastsorcererspat0000morr |url-access=registration |publisher=Joseph Henry Press
 |isbn=978-0-309-50593-2
}}

== External links ==
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{{Fundamental interactions}}
{{Standard model of physics}}

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[[Category:Fundamental interactions]]
[[Category:Nuclear physics]]
[[Category:Quantum chromodynamics]]