Generation (particle physics)
Topic: Physics
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In particle physics, a generation or family is a division of the elementary particles. Between generations, particles differ by their flavour quantum number and mass, but their electric and strong interactions are identical.
There are three generations according to the Standard Model of particle physics. Each generation contains two types of leptons and two types of quarks. The two leptons may be classified into one with electric charge −1 (electron-like) and neutral (neutrino); the two quarks may be classified into one with charge −1⁄3 (down-type) and one with charge +2⁄3 (up-type). The basic features of quark–lepton generation or families, such as their masses and mixings etc., can be described by some of the proposed family symmetries.
| Type | Generations of matter | ||
|---|---|---|---|
| First | Second | Third | |
| Quarks | |||
| up-type | up | charm | top |
| down-type | down | strange | bottom |
| Leptons | |||
| charged | electron | muon | tau |
| neutral | electron neutrino | muon neutrino | tau neutrino |
Overview
Each member of a higher generation has greater mass than the corresponding particle of the previous generation, with the possible exception of the neutrinos (whose small but non-zero masses have not been accurately determined). For example, the first-generation electron has a mass of only 0.511 MeV/c2, the second-generation muon has a mass of 106 MeV/c2, and the third-generation tau has a mass of 1777 MeV/c2 (almost twice as heavy as a proton). This mass hierarchy[1] causes particles of higher generations to decay to the first generation, which explains why everyday matter (atoms) is made of particles from the first generation only. Electrons surround a nucleus made of protons and neutrons, which contain up and down quarks. The second and third generations of charged particles do not occur in normal matter and are only seen in extremely high-energy environments such as cosmic rays or particle accelerators. The term generation was first introduced by Haim Harari in Les Houches Summer School, 1976.[2][3]
Neutrinos of all generations stream throughout the universe but rarely interact with other matter.[4] It is hoped that a comprehensive understanding of the relationship between the generations of the leptons may eventually explain the ratio of masses of the fundamental particles, and shed further light on the nature of mass generally, from a quantum perspective.[5]
Fourth generation
Fourth and further generations are considered unlikely by many (but not all) theoretical physicists. Some arguments against the possibility of a fourth generation are based on the subtle modifications of precision electroweak observables that extra generations would induce; such modifications are strongly disfavored by measurements. Furthermore, a fourth generation with a 'light' neutrino (one with a mass less than about 45 GeV/c2) has been ruled out by measurements of the decay widths of the Z boson at CERN's Large Electron–Positron Collider (LEP).[6] Nonetheless, searches at high-energy colliders for particles from a fourth generation continue, but as yet no evidence has been observed.[7] In such searches, fourth-generation particles are denoted by the same symbols as third-generation ones with an added prime (e.g. b′ and t′).
The lower bound for a fourth generation of quark (b′, t′) masses is currently at 1.4 TeV from experiments at the LHC.[8]
The lower bound for a fourth generation neutrino ([math]\displaystyle{ ~\nu_{\tau}'~ }[/math]) mass is currently at about 60 GeV (millions of times larger than the upper bound for the other 3 neutrino masses).[9]
The lower bound for a fourth generation charged lepton ([math]\displaystyle{ \tau' }[/math]) mass is currently 100GeV and proposed upper bound of 1.2 TeV from unitarity considerations.[10]
If the Koide formula continues to hold, the masses of the fourth generation charged lepton would be 44 GeV (ruled out) and b′ and t′ should be 3.6 TeV and 84 TeV respectively. (The maximum possible energy for protons in the LHC is about 6 TeV.)
Origin
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Unsolved problem in physics: Why are there three generations of quarks and leptons? Is there a theory that can explain the masses of particular quarks and leptons in particular generations from first principles (a theory of Yukawa couplings)? (more unsolved problems in physics)
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The origin of multiple generations of fermions, and the particular count of 3, is an unsolved problem of physics. String theory provides a cause for multiple generations, but the particular number depends on the details of the compactification of the D-brane intersections. Additionally, E8 grand unified theories in 10 dimensions compactified on certain orbifolds down to 4‑D naturally contain 3 generations of matter.[11] This includes many heterotic string theory models. In standard quantum field theory, under certain assumptions, a single fermion field can give rise to multiple fermion poles with mass ratios of around eπ≈23 and e2π≈535 potentially explaining the large ratios of fermion masses between successive generations and their origin.[1]
See also
References
- ↑ 1.0 1.1 Blumhofer, A.; Hutter, M. (1997). "Family structure from periodic solutions of an improved gap equation". Nuclear Physics B 484 (1): 80–96. doi:10.1016/S0550-3213(96)00644-X. Bibcode: 1997NuPhB.484...80B. (Erratum: doi:10.1016/S0550-3213(97)00228-9)
- ↑ Harari, H. (5 July – 14 August 1976). "Beyond charm". in Balian, R.; Llewellyn-Smith, C.H.. Weak and Electromagnetic Interactions at High Energy. 29. Les Houches, France: North-Holland. 1977. p. 613. http://www.slac.stanford.edu/spires/find/hep/www?irn=154660.
- ↑ Harari, H. (1977). "Three generations of quarks and leptons". p. 170. SLAC-PUB-1974. http://slac.stanford.edu/cgi-wrap/getdoc/slac-pub-1974.pdf.
- ↑ "Experiment confirms famous physics model". MIT Press Office (Press release). Massachusetts Institute of Technology. 18 April 2007.
- ↑ Mac Gregor, M.H. (2006). "A 'muon mass tree' with α‑quantized lepton, quark, and hadron masses". arXiv:hep-ph/0607233.CS1 maint: multiple names: authors list (link)
- ↑ Decamp, D. (1989). "Determination of the number of light neutrino species". Physics Letters B 231 (4): 519–529. doi:10.1016/0370-2693(89)90704-1. Bibcode: 1989PhLB..231..519D. https://cds.cern.ch/record/201511.
- ↑ Amsler, C. (2008). "b′ (4th Generation) Quarks, searches for". Physics Letters B. Review of Particle Physics 667 (1): 1–1340. doi:10.1016/j.physletb.2008.07.018. Bibcode: 2008PhLB..667....1A. http://pdg.lbl.gov/2008/listings/q008.pdf.
- ↑ CMS Collaboration (8 May 2019). "Boosting searches for fourth-generation quarks". CERN Courier. https://cerncourier.com/a/boosting-searches-for-fourth-generation-quarks/.
- ↑ Carpenter, Linda M.; Rajaraman, Arvind (December 2010). "Revisiting constraints on fourth generation neutrino masses". Physical Review D 82 (11): 114019. doi:10.1103/PhysRevD.82.114019. Bibcode: 2010PhRvD..82k4019C. "ABSTRACT: We revisit the current experimental bounds on fourth-generation Majorana neutrino masses, including the effects of right handed neutrinos. Current bounds from LEP‑II are significantly altered by a global analysis. We show that the current bounds on fourth generation neutrinos decaying to e W and μ W can be reduced to about 80 GeV (from the current bound of 90 GeV), while a neutrino decaying to τ W can be as light as 62.1 GeV. The weakened bound opens up a neutrino decay channel for intermediate mass Higgs, and interesting multi-particle final states for Higgs and fourth generation lepton decays.".
- ↑ Dighe, Amol; Ghosh, Diptimoy; Godbole, Rohini M.; Prasath, Arun (2012). "Large mass splittings for fourth generation fermions allowed by LHC Higgs boson exclusion". Physical Review D 85 (11): 114035. doi:10.1103/PhysRevD.85.114035. Bibcode: 2012PhRvD..85k4035D.
- ↑ Motl, Luboš (13 July 2021). "The "pure joy" E8 SUSY toroidal orbifold TOE". https://motls.blogspot.com/2021/07/the-pure-joy-e8-susy-toroidal-orbifold.html.
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