View source for Preon

{{Short description|Hypothetical subatomic particle}}
{{for multi|the infectious proteins|Prion|the chemical pollutants|Chlorofluorocarbon}}
 
In [[particle physics]], '''preons''' are hypothetical [[point particle]]s, conceived of as sub-components of [[quark]]s and [[lepton]]s.<ref name="D'Souza">
{{cite book
 |last1=D'Souza |first1=I.A.
 |last2=Kalman |first2=C.S.
 |year=1992
 |title=Preons: Models of Leptons, Quarks and Gauge Bosons as Composite Objects
 |publisher=[[World Scientific]]
 |isbn=978-981-02-1019-9
}}</ref> The word was coined by [[Jogesh Pati]] and [[Abdus Salam]], in 1974. Interest in preon models peaked in the 1980s but has slowed, as the [[Standard Model]] of particle physics continues to describe physics mostly successfully, and no direct experimental evidence for lepton and quark compositeness has been found. Preons come in four varieties: plus, anti-plus, zero, and anti-zero. [[W boson]]s have six preons, and quarks and leptons have only three. 

In the [[hadron]]ic sector, some effects are considered anomalies within the Standard Model. For example, the [[proton spin crisis|proton spin puzzle]], the [[EMC effect]], the distributions of electric charges inside the [[nucleon]]s, as found by [[Robert Hofstadter]] in 1956,<ref>{{cite journal |last1=Hofstadter |first1=Robert |date=1 July 1956 |title=Electron Scattering and Nuclear Structure |journal=Reviews of Modern Physics |volume=28 |issue=3 |pages=214–254 |doi=10.1103/RevModPhys.28.214 |bibcode=1956RvMP...28..214H }}</ref><ref>{{cite journal |last1=Hofstadter |first1=R. |last2=Bumiller |first2=F. |last3=Yearian |first3=M.R. |date=1 April 1958 |title=Electromagnetic Structure of the Proton and Neutron |journal=Reviews of Modern Physics |volume=30 |issue=2 |pages=482–497 |doi=10.1103/RevModPhys.30.482 |bibcode=1958RvMP...30..482H  |url=http://www.physics.princeton.edu/~mcdonald/examples/EP/hofstadter_rmp_30_482_58.pdf |archive-url=https://web.archive.org/web/20180223210328/http://www.physics.princeton.edu/~mcdonald/examples/EP/hofstadter_rmp_30_482_58.pdf |archive-date=2018-02-23 |url-status=live}}</ref> and the ad hoc [[CKM matrix]] elements.

When the term "preon" was coined, it was primarily to explain the two families of spin-{{Sfrac|1|2}} fermions: quarks and leptons. More recent preon models also account for spin-1 bosons, and are still called "preons". Each of the preon models postulates a set of fewer fundamental particles than those of the Standard Model, together with the rules governing how those fundamental particles combine and interact. Based on these rules, the preon models try to explain the Standard Model, often predicting small discrepancies with this model and generating new particles and certain phenomena which do not belong to the Standard Model.

==Goals of preon models==
Preon research is motivated by the desire to:
* Reduce the large number of particles, many that differ only in charge, to a smaller number of more fundamental particles. For example, the [[down quark]] and [[up quark]] are nearly identical except for charge, and a slight mass difference; preon research is motivated by explaining that quarks are composed of similar preons, with incremental differences accounting for charge. The hope is to reproduce the [[reductionist]] strategy that has worked for the [[periodic table of elements]] and the [[quark model]] of mesons and baryons.
* Explain the reason for there being exactly three [[Generation (particle physics)|generation]]s of [[fermions]].
* Calculate parameters that are currently unexplained by the Standard Model, such as the [[mass]]es of S.M. fundamental fermions, their [[electric charge]]s, and [[color charge]]s; in effect, reduce the number of model-required experimental input parameters from the number required by the Standard Model.
* Provide reasons for the very large range of mass-energy observed in supposedly fundamental particles, from the [[electron neutrino]] to the [[top quark]].
* Provide alternative explanations for the [[electro-weak]] [[symmetry breaking]] without invoking a [[Higgs field]], which itself possibly needs a [[supersymmetry]] to correct the theoretical problems involved with the Higgs field;{{which|date=February 2016}} (further, the supersymmetric theories proposed so far have theoretical and observational problems of their own{{which|date=February 2016}}).
* Account for [[neutrino oscillation]] and apparently [[neutrino#neutrino_mass_anchor|unique mass mechanism]].
* Make new, non-repetitive predictions, such as providing [[cold dark matter]] candidates.
* Explain why there exists only the observed variety of particle species, and give a model with reasons for producing ''only'' these observed particles (since the prediction of non-observed particles is a problem with many current models, such as [[supersymmetry]]).

==Background==
Before the Standard Model was developed in the 1970s (the key elements of the Standard Model known as [[quark]]s were proposed by [[Murray Gell-Mann]] and [[George Zweig]] in 1964), physicists observed hundreds of different kinds of particles in [[particle accelerator]]s. These were organized into relationships on their physical properties in a largely ad-hoc system of hierarchies, not entirely unlike the way [[Taxonomy (biology)|taxonomy]] grouped animals based on their physical features. Not surprisingly, the huge number of particles was referred to as the "[[particle zoo]]".

The Standard Model, which is now the prevailing model of particle physics, dramatically simplified this picture by showing that most of the observed particles were [[meson]]s, which are combinations of two [[quark]]s, or [[baryon]]s which are combinations of three quarks, plus a handful of other particles. The particles being seen in the ever-more-powerful accelerators were, according to the theory, typically nothing more than combinations of these quarks.

===Comparisons of quarks, leptons, and bosons===
Within the Standard Model, there are [[List of particles|several classes of particles]]. One of these, the [[quark]]s, has six types, of which there are three varieties in each (dubbed "[[Color charge|colors]]", red, green, and blue, giving rise to [[quantum chromodynamics]]).

Additionally, there are six different types of what are known as [[lepton]]s. Of these six leptons, there are three [[charged particle]]s: the [[electron]], [[muon]], and [[tau (particle)|tau]]. The [[neutrino]]s comprise the other three leptons, and each neutrino pairs with one  of the three charged leptons.

In the Standard Model, there are also [[boson]]s, including the [[photon]]s and [[gluon]]s; [[W and Z bosons|W{{sup|+}}, W{{sup|−}}, and Z bosons]]; and the [[Higgs boson]]; and an open space left for the [[graviton]]. Almost all of these particles come in "left-handed" and "right-handed" versions (see '' [[Chirality (physics)|chirality]]''). The quarks, leptons, and W boson all have [[antiparticle]]s with opposite electric charge (or in the case of the neutrinos, opposite [[weak isospin]]).

===Unresolved problems with the Standard Model===
The Standard Model also has a number of problems which have not been entirely solved. In particular, no successful theory of [[gravitation]] based on a particle theory has yet been proposed. Although the Model assumes the existence of a graviton, all attempts to produce a consistent theory based on them have failed.

Kalman<ref>{{cite journal |last=Kalman |first=C.S. |year=2005 |title=Why quarks cannot be fundamental particles |journal=Nuclear Physics B: Proceedings Supplements |volume=142 |pages=235–237 |doi=10.1016/j.nuclphysbps.2005.01.042 |arxiv=hep-ph/0411313 |bibcode=2005NuPhS.142..235K |s2cid=119394495 }}</ref> asserts that, according to the concept of [[atomism]], fundamental building blocks of nature are indivisible bits of matter that are ungenerated and indestructible. Neither leptons nor quarks are truly indestructible, since some leptons can decay into other leptons, some quarks into other quarks. Thus, on fundamental grounds, quarks are not themselves fundamental building blocks, but must be composed of other, fundamental quantities—preons. Although the mass of each successive particle follows certain patterns, predictions of the [[rest mass]] of most particles cannot be made precisely, except for the masses of almost all baryons which have been modeled well by de&nbsp;Souza (2010).<ref>{{cite journal |last=de&nbsp;Souza |first=Mario Everaldo  |year=2010 |title=Calculation of almost all energy levels of baryons |journal=[[Papers in Physics]] |volume=3 |pages=030003–1 |doi=10.4279/PIP.030003 |url=http://www.papersinphysics.org/papersinphysics/article/download/64/pdf64 |doi-access=free }}</ref>

The Standard Model also has problems predicting the large scale structure of the universe. For instance, the SM generally predicts equal amounts of matter and [[antimatter]] in the universe. A number of attempts have been made to "fix" this through a variety of mechanisms, but to date none have won widespread support. Likewise, basic adaptations of the Model suggest the presence of [[proton decay]], which has not yet been observed.

===Motivation for preon models===
Several models have been proposed in an attempt to provide a more fundamental explanation of the results in experimental and theoretical particle physics, using names such as "[[Parton (particle physics)|parton]]" or "preon" for the hypothetical basic particle constituents.

Preon theory is motivated by a desire to replicate in particle physics the achievements of the [[periodic table]] in Chemistry, which reduced 94&nbsp;naturally occurring elements to combinations of just three building-blocks (proton, neutron, electron). Likewise, the [[Standard Model]] later organized the "particle zoo" of [[hadrons]] by reducing several dozen particles to combinations at a more fundamental level of (at first) just three [[quarks]], consequently reducing the huge number of arbitrary constants in mid-twentieth-century particle physics prior to the [[Standard Model]] and [[quantum chromodynamics]].

However, the particular preon model discussed below has attracted comparatively little interest among the particle physics community to date, in part because no evidence has been obtained so far in collider experiments to show that the fermions of the Standard Model are composite.

===Attempts===
A number of physicists have attempted to develop a theory of "pre-quarks" (from which the name ''preon'' derives) in an effort to justify theoretically the many parts of the Standard Model that are known only through experimental data. Other names which have been used for these proposed fundamental particles (or particles intermediate between the most fundamental particles and those observed in the Standard Model) include ''prequarks'', ''subquarks'', ''maons'',<ref>
{{cite news
 |last=Overbye |first=D. |author-link=Dennis Overbye
 |date=5 December 2006
 |title=China pursues major role in particle physics
 |newspaper=[[The New York Times]]
 |url=https://www.nytimes.com/2006/12/05/science/05china.html
 |access-date=2011-09-12
}}
</ref> ''alphons'', ''quinks'', ''[[Rishon model|rishon]]s'', ''tweedles'', ''helons'', ''haplons'', ''Y-particles'',<ref>
{{cite journal
 |last1=Yershov |first=V.N.
 |year=2005
 |title=Equilibrium configurations of tripolar charges
 |journal=[[Few-Body Systems]]
 |volume=37 |issue=1–2 |pages=79–106
 |arxiv=physics/0609185 |bibcode = 2005FBS....37...79Y
 |doi=10.1007/s00601-004-0070-2 |s2cid=119474883
}}
</ref> and ''primons''.<ref>
{{cite journal
 |last1=de Souza |first1=M.E.
 |year=2005
 |title=The ultimate division of matter
 |journal=[[Scientia Plena]]
 |volume=1 |issue=4 |pages=83
}}
</ref> ''Preon'' is the leading name in the physics community.

Efforts to develop a substructure date at least as far back as 1974 with a paper by Pati and Salam in ''[[Physical Review]]''.<ref>
{{cite journal
 |last1=Pati  |first1=J.C.
 |last2=Salam |first2=A.
 |year=1974
 |title=Lepton number as the fourth "color"
 |journal=[[Physical Review D]]
 |volume=10 |issue=1 |pages=275–289
 |bibcode = 1974PhRvD..10..275P |doi=10.1103/PhysRevD.10.275
 |s2cid=17349483
 |url=http://pdfs.semanticscholar.org/21fb/f9d49acf3e3f07098ca686ae4058c38dbd03.pdf
 |url-status=dead
 |archive-url=https://web.archive.org/web/20190220013017/http://pdfs.semanticscholar.org/21fb/f9d49acf3e3f07098ca686ae4058c38dbd03.pdf
 |archive-date=2019-02-20
}}<br/>Erratum:
{{cite journal
 |last1=Pati  |first1=J.C.
 |last2=Salam |first2=A.
 |year=1975
 |title=Erratum: Lepton number as the fourth "color"
 |journal=[[Physical Review D]]
 |volume=11 |issue=3 |page=703
 |bibcode = 1975PhRvD..11..703P |doi=10.1103/PhysRevD.11.703.2
|doi-access=free}}
</ref>
Other attempts include a 1977 paper by Terazawa, Chikashige, and Akama,<ref>
{{cite journal
 |last1=Terazawa   |first1=H.
 |last2=Chikashige |first2=Y.
 |last3=Akama      |first3=K.
 |year=1977
 |title=Unified model of the Nambu-Jona-Lasinio type for all elementary particles
 |journal=[[Physical Review D]]
 |volume=15 |issue=2 |pages=480–487
 |bibcode = 1977PhRvD..15..480T  |doi=10.1103/PhysRevD.15.480
}}
</ref> similar, but independent, 1979 papers by Ne'eman,<ref>
{{cite journal
 |last=Ne'eman |first=Y.
 |year=1979
 |title=Irreducible gauge theory of a consolidated Weinberg-Salam model
 |journal=[[Physics Letters B]]
 |volume=81 |issue=2 |pages=190–194 
 |bibcode = 1979PhLB...81..190N  |osti=6534180
 |doi=10.1016/0370-2693(79)90521-5
 |url=https://www.osti.gov/biblio/6534180
}}
</ref>
Harari,<ref name=harari1>
{{cite journal
 |last=Harari |first=H.
 |year=1979
 |title=A schematic model of quarks and leptons
 |url=http://www.slac.stanford.edu/cgi-wrap/getdoc/slac-pub-2310.pdf
 |journal=[[Physics Letters B]]
 |volume=86 |issue=1 |pages=83–86
 |bibcode = 1979PhLB...86...83H |osti=1447265 
 |doi=10.1016/0370-2693(79)90626-9
}}</ref>
and Shupe,<ref>
{{cite journal
 |last=Shupe |first=M.A.
 |year=1979
 |title=A composite model of leptons and quarks
 |journal=[[Physics Letters B]]
 |volume=86 |issue=1 |pages=87–92
 |bibcode=1979PhLB...86...87S
 |doi=10.1016/0370-2693(79)90627-0
}}
</ref> a 1981 paper by Fritzsch and Mandelbaum,<ref>
{{cite journal
 |last1=Fritzsch   |first1=H.
 |last2=Mandelbaum |first2=G.
 |year=1981
 |title=Weak interactions as manifestations of the substructure of leptons and quarks
 |journal=[[Physics Letters B]]
 |volume=102 |issue=5 |pages=319
 |bibcode = 1981PhLB..102..319F
 |doi=10.1016/0370-2693(81)90626-2
}}
</ref>
and a 1992 book by D'Souza and Kalman.<ref name="D'Souza"/> None of these have gained wide acceptance in the physics world. However, in a recent work<ref>
{{cite journal
 |last=de&nbsp;Souza |first=M.E.
 |year=2008
 |title=Weak decays of hadrons reveal compositeness of quarks
 |journal=[[Scientia Plena]]
 |volume=4 |issue=6 |pages=064801–1
}}</ref>
de&nbsp;Souza has shown that his model describes well all weak decays of hadrons according to selection rules dictated by a quantum number derived from his compositeness model. In his model leptons are elementary particles and each quark is composed of two ''primons'', and thus, all quarks are described by four ''primons''. Therefore, there is no need for the Standard Model Higgs boson and each quark mass is derived from the interaction between each pair of ''primons'' by means of three Higgs-like bosons.

In his 1989 [[Nobel Prize]] acceptance lecture, [[Hans Georg Dehmelt|Hans Dehmelt]] described a most fundamental elementary particle, with definable properties, which he called the ''[[cosmon]]'', as the likely result of a long but finite chain of increasingly more elementary particles.<ref>
{{cite web
 |last=Dehmelt |first=H.G.
 |year=1989
 |title=Experiments with an isolated subatomic particle at rest
 |series=Nobel lecture
 |publisher=[[The Nobel Foundation]]
 |url=https://www.nobelprize.org/nobel_prizes/physics/laureates/1989/dehmelt-lecture.html
}} See also references therein.
</ref>

===Composite Higgs===
{{See also|Composite Higgs models|Two-Higgs-doublet model}}{{update|date=July 2019}}
Many preon models either do not account for the [[Higgs boson]] or rule it out, and propose that electro-weak symmetry is broken not by a scalar Higgs field but by composite preons.<ref>{{cite arXiv |last1=Dugne |first1=J.-J. |last2=Fredriksson |first2=S. |last3=Hansson |first3=J. |last4=Predazzi |first4=E. |year=1997 |title=Higgs pain? Take a preon! |eprint=hep-ph/9709227}}</ref>  For example, Fredriksson preon theory does not need the Higgs boson, and explains the electro-weak breaking as the rearrangement of preons, rather than a Higgs-mediated field. In fact, the Fredriksson preon model and the de Souza model predict that the Standard Model Higgs boson does not exist.

==Rishon model==
{{Main|Rishon model}}
The ''[[rishon model]]'' (RM) is the earliest effort (1979) to develop a preon model to explain the phenomenon appearing in the [[Standard Model]] (SM) of [[particle physics]]. It was first developed by [[Haim Harari]] and Michael A. Shupe (independently of each other), and later expanded by Harari and his then-student [[Nathan Seiberg]].<ref name=HarariSeiberg1984>{{cite journal
 |last1=Harari
 |first1=Haim
 |last2=Seiberg
 |first2=Nathan
 |year=1982
 |title=The Rishon model
 |journal=Nuclear Physics B
 |volume=204
 |issue=1
 |pages=141–167
 |publisher=North-Holland Publishing
 |bibcode=1982NuPhB.204..141H
 |doi=10.1016/0550-3213(82)90426-6
 |url=http://www.weizmann.ac.il/home/harari/files/Nuclear_PhysicsB_Vol204.pdf
 |access-date=2018-06-02
 |archive-date=2012-10-07
 |archive-url=https://web.archive.org/web/20121007014745/http://www.weizmann.ac.il/home/harari/files/Nuclear_PhysicsB_Vol204.pdf
 |url-status=dead
 }}</ref>

The model has two kinds of fundamental particles called '''rishons''' (ראשונים, which means "First" in [[Hebrew]]). They are '''T''' ("Third" since it has an electric charge of ⅓&nbsp;[[elementary charge|''e'']], or Tohu (תוהו) which means [[Tohu va bohu|"Chaos"]]) and '''V''' ("Vanishes",  since it is electrically neutral, or Vohu which means "void"). All [[lepton]]s and all [[flavour (particle physics)|flavour]]s of [[quark]]s are three-rishon ordered triplets. These groups of three rishons have [[spin-½]].

The [[Rishon model]] illustrates some of the typical efforts in the field. Many of the preon models theorize that the apparent imbalance of matter and antimatter in the universe is in fact illusory, with large quantities of preon-level antimatter confined within more complex structures.

==Criticisms==

===The mass paradox===
One preon model started as an internal paper at the Collider Detector at [[Fermilab]] (CDF) around 1994.<ref name=cramer>{{cite web
|last=Cramer
|first=John G.
|title=Alternative View: A Different Approach to Particle Physics
|url=https://www.npl.washington.edu/av/altvw80.html
|website=Nuclear Physics Laboratory, University of Washington
|date=August 1980
|access-date=1 July 2024
}}</ref> The paper was written after an unexpected and inexplicable excess of jets with energies above 200 [[electronvolt|GeV]] were detected in the 1992–1993 running period. However, [[scattering]] experiments have shown that quarks and leptons are "point like" down to distance scales of less than {{10^|−18}} m (or {{frac|1|1000}} of a proton diameter).<ref>{{cite journal
|last=Riordan
|first=Michael
|title=The Search for Quark Compositeness
|journal=Annual Review of Nuclear and Particle Science
|date=1992
|volume=42
|pages=1–32
|doi=10.1146/annurev.ns.42.120192.000245
}}</ref> The [[momentum]] [[uncertainty]] of a preon (of whatever mass) confined to a box of this size is about 200 GeV/c, which is 50,000 times larger than the (model dependent) [[rest mass]] of an up-quark, and 400,000 times larger than the rest mass of an electron.

Heisenberg's [[uncertainty principle]] states that <math>\operatorname{\Delta} x \cdot \operatorname{\Delta} p \ge \tfrac{1}{2}\hbar</math> and thus anything confined to a box smaller than <math>\operatorname{\Delta} x</math> would have a momentum uncertainty proportionally greater. For preons confined within quarks or leptons (Δx ~10⁻¹⁸ m), this implies kinetic energies ~200 GeV—far exceeding observed quark/lepton masses.<ref name=cramer/>

So the preon model represents a mass paradox: How could quarks or electrons be made of smaller particles that would have many orders of magnitude greater mass-energies arising from their enormous momenta? One way of resolving this paradox is to postulate a large binding force between preons that cancels their mass-energies. For example, some models propose a "hyperstrong" interaction ~100,000 times stronger than the nuclear strong force to negate the preons’ kinetic contributions.<ref>{{cite journal
|last=Harari
|first=Haim
|title=The Structure of Quarks and Leptons
|journal=Physics Letters B
|date=1979
|volume=86
|issue=1
|pages=83–86
|doi=10.1016/0370-2693(79)90626-9
}}</ref>

===Conflicts with observed physics===
Preon models propose additional unobserved forces or dynamics to account for the observed properties of elementary particles, which may have implications in conflict with observation. For example, now that the [[Large Hadron Collider|LHC]]'s observation of a [[Higgs boson]] is confirmed, the observation contradicts the predictions of many preon models that excluded it.<ref name=harari1/><ref>{{cite journal |author=Fritzsch, H. and Mandelbaum, G. |title=Weak Interactions as Manifestations of the Substructure of Leptons and Quarks |journal=Physics Letters B |date=1981 |volume=102 |pages=319–322 }}</ref>

Preon theories require quarks and leptons to have a finite size. It is possible that the [[Large Hadron Collider]] will observe this after it is upgraded to higher energies.<ref>{{cite journal |author=Eichten, E.; Lane, K.; Peskin, M. E. |title=New Tests for Quark and Lepton Substructure |journal=Physical Review Letters |date=1983 |volume=50 |pages=811–814 |doi=10.1103/PhysRevLett.50.811 }}</ref>

==In popular culture==
{{unreferenced section|date=November 2022}}
* In the 1948 reprint/edit of his 1930 novel ''[[Skylark of Space|Skylark Three]]'', [[E. E. Smith]] postulated a series of 'subelectrons of the first and second type' with the latter being fundamental particles that were associated with the gravitation force. While this may not have been an element of the original novel (the scientific basis of some of the other novels in the series was revised extensively due to the additional eighteen years of scientific development), even the edited publication may be the first, or one of the first, mentions of the possibility that electrons are not fundamental particles.
* In the novelized version of the 1982 motion picture ''[[Star Trek II: The Wrath of Khan]]'', written by [[Vonda McIntyre]], two of Dr. Carol Marcus' Genesis project team, Vance Madison and Delwyn March, have studied sub-elementary particles they've named "boojums" and "snarks", in a field they jokingly call "kindergarten physics" because it is lower than "elementary" (analogy to school levels).
* [[James P. Hogan (writer)|James P. Hogan]]'s 1982 novel ''[[Voyage from Yesteryear]]'' discussed preons (called ''tweedles''), the physics of which became central to the plot.
* In the 2018 VR video game ''[[Blade and Sorcery]]'', a preon star is revealed to be the energy source that powers magic in the game's world, and its 10,000 year close orbital pass is a key driver for the plot.
* In the 2020 video game ''[[Risk of Rain 2]]'', an item in the game is called the 'preon accumulator', though only a reference in name.

==See also==
* {{Annotated link|Technicolor (physics)}}
* {{Annotated link|Preon star}}
* {{Annotated link|Preon-degenerate matter}}
* {{Annotated link|Rishon model}}

==References==
{{reflist|25em}}

==Further reading==
* {{cite news
 |last1=Ball |first=P.
 |year=2007
 |title=Splitting the quark
 |journal=[[Nature (journal)|Nature]]
 |doi=10.1038/news.2007.292
}}
* {{cite web
 |first=Robert |last=Piccioni
 |date=2013-01-07
 |title=Have we hit bottom yet?
 |series=newsletter
 |website=guidetothecosmos.com
 |url=https://guidetothecosmos.com/newsletter-HitBottom.html
}} — an editorial about preons

{{particles}}

[[Category:Hypothetical elementary particles]]