subatomic particle

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subatomic particle
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{{short description|Particle whose size or mass is less than that of the atom, or of which the atom is composed; small quantum particle}}{{pp-move-indef}}{{Standard model of particle physics}}In the physical sciences, subatomic particles are particles much smaller than atoms.WEB, Subatomic particles,weblink NTD, 5 June 2012, The two types of subatomic particles are: elementary particles, which according to current theories are not made of other particles; and composite particles.BOOK, Bolonkin, Alexander, Universe, Human Immortality and Future Human Evaluation, 2011, Elsevier, 9780124158016, 25, Particle physics and nuclear physics study these particles and how they interact.BOOK
, Fritzsch, Harald
, 2005
, Elementary Particles
, 11–20
, World Scientific
, 978-981-256-141-1
, The idea of a particle underwent serious rethinking when experiments showed that light could behave like a stream of particles (called photons) as well as exhibiting wave-like properties. This led to the new concept of wave–particle duality to reflect that quantum-scale "particles" behave like both particles and waves (they are sometimes described as wavicles to reflect this). Another new concept, the uncertainty principle, states that some of their properties taken together, such as their simultaneous position and momentum, cannot be measured exactly.{{Citation |first=W. |last=Heisenberg |title=Über den anschaulichen Inhalt der quantentheoretischen Kinematik und Mechanik |language=de|journal=Zeitschrift für Physik |volume=43 |issue=3–4 |date=1927 |pages=172–198 |doi=10.1007/BF01397280 |postscript=. |bibcode = 1927ZPhy...43..172H }} In more recent times, wave–particle duality has been shown to apply not only to photons but to increasingly massive particles as well.JOURNAL
, 2000
, Wave-particle duality of C60 molecules
, Anton
, Zeilinger
, Gerbrand
, Van Der Zouw
, Claudia
, Keller
, Julian
, Nature (journal), Nature
, Vos-Andreae
, 401
, Olaf
, 10.1038/44348
, Nairz
, 1999Natur.401..680A, 6754, 680–682
, Arndt
, Markus, 18494170
, Interactions of particles in the framework of quantum field theory are understood as creation and annihilation of quanta of corresponding fundamental interactions. This blends particle physics with field theory.


By composition

Subatomic particles are either "elementary", i.e. not made of multiple other particles, or "composite" and made of more than one elementary particle bound together.
The elementary particles of the Standard Model are:BOOK
, Cottingham, W.N.
, Greenwood, D.A.
, 2007
, An introduction to the standard model of particle physics
, Cambridge University Press
, 1
, 978-0-521-85249-4
, File:Standard Model of Elementary Particles.svg|thumb|392x392px|The Standard ModelStandard ModelAll of these have now been discovered by experiments, with the latest being the top quark (1995), tau neutrino (2000), and Higgs boson (2012). Various extensions of the Standard Model predict the existence of an elementary graviton particle and many other elementary particles, but none have been discovered as of 2019.


Nearly all composite particles contain multiple quarks (antiquarks) bound together by gluons (with a few exceptions with no quarks, such as positronium and muonium). Those containing few (≤ 5) [anti]quarks are called hadrons. Due to a property known as color confinement, quarks are never found singly but always occur in hadrons containing multiple quarks. The hadrons are divided by number of quarks (including antiquarks) into the baryons containing an odd number of quarks (almost always 3), of which the proton and neutron (the two nucleons) are by far the best known; and the mesons containing an even number of quarks (almost always 2, one quark and one antiquark), of which the pions and kaons are the best known. Except for the proton and neutron, all other hadrons are unstable and decay into other particles in microseconds or less. A proton is made of two up quarks and one down quark, while the neutron is made of two down quarks and one up quark. These commonly bind together into an atomic nucleus, e.g. a helium-4 nucleus is composed of two protons and two neutrons. Most hadrons do not live long enough to bind into nucleus-like composites; those who do (other than the proton and neutron) form exotic nuclei.

By statistics

Any subatomic particle, like any particle in the three-dimensional space that obeys the laws of quantum mechanics, can be either a boson (with integer spin) or a fermion (with odd half-integer spin). In the Standard Model, all the elementary fermions have spin 1/2, and are divided into the quarks which carry color charge and therefore feel the strong interaction, and the leptons which do not. The elementary bosons comprise the gauge bosons (photon, W and Z, gluons) with spin 1, while the Higgs boson is the only elementary particle with spin zero. The hypothetical graviton is required theoretically to have spin 2, but is not part of the Standard Model. Some extensions such as supersymmetry predict additional elementary particles with spin 3/2, but none have been discovered as of 2019.Due to the laws for spin of composite particles, the baryons (3 quarks) have spin either 1/2 or 3/2, and are therefore fermions; the mesons (2 quarks) have integer spin of either 0 or 1, and are therefore bosons.

By mass

In special relativity, the energy of a particle at rest equals its mass times the speed of light squared, {{nowrap begin}}E = mc2{{nowrap end}}. That is, mass can be expressed in terms of energy and vice versa. If a particle has a frame of reference in which it lies at rest, then it has a positive rest mass and is referred to as massive.All composite particles are massive. Baryons (meaning "heavy") tend to have greater mass than mesons (meaning "intermediate"), which in turn tend to be heavier than leptons (meaning "lightweight"), but the heaviest lepton (the tau particle) is heavier than the two lightest flavours of baryons (nucleons). It is also certain that any particle with an electric charge is massive. When originally defined in the 1950s, the terms baryons, mesons and leptons referred to masses; however, after the quark model became accepted in the 1970s, it was recognised that baryons are composites of three quarks, mesons are composites of one quark and one antiquark, while leptons are elementary and are defined as the elementary fermions with no color charge. All massless particles (particles whose invariant mass is zero) are elementary. These include the photon and gluon, although the latter cannot be isolated.

By decay

Most subatomic particles are not stable. All mesons, as well as baryons—except for proton—decay by either strong or weak force. Proton observationally doesn't decay, although whether is it "truly" stable is unknown. Charged leptons mu and tau decay by weak force; the same for their antiparticles. Neutrinos (and antineutrinos) don't decay, but a related phenomenon of neutrino oscillations is thought to exist even in vacuum. Electron and its antiparticle positron are theoretically stable due to charge conservation unless a lighter particle having magnitude of electric charge {{abbr|≤|less than or equal}} e exists (which is unlikely).Of subatomic particles which don't carry color (and hence can be isolated) only photon, electron, neutrinos with someIf there are three sorts of neutrino having a well-defined invariant mass, then mass eigenstates are stable, but they don't correspond to flavor eigenstates. disclaimers, several atomic nuclei (proton included), and antiparticles thereof can remain in the same state indefinitely.

Other properties

All observable subatomic particles have their electric charge an integer multiple of the elementary charge. The Standard Model's quarks have "non-integer" electric charges, namely, multiple of {{frac|1|3}} e, but quarks (and other combinations with non-integer electric charge) cannot be isolated due to color confinement. For baryons, mesons, and their antiparticles the constituent quarks' charges sum up to an integer multiple of e.Through the work of Albert Einstein, Satyendra Nath Bose, Louis de Broglie, and many others, current scientific theory holds that all particles also have a wave nature.BOOK
, Walter Greiner
, 2001
, Quantum Mechanics: An Introduction
, 29
, Springer (publisher), Springer
, 978-3-540-67458-0
, This has been verified not only for elementary particles but also for compound particles like atoms and even molecules. In fact, according to traditional formulations of non-relativistic quantum mechanics, wave–particle duality applies to all objects, even macroscopic ones; although the wave properties of macroscopic objects cannot be detected due to their small wavelengths.BOOK
, Eisberg, R.
, Resnick, R.
, yes
, 1985
, Quantum Physics of Atoms, Molecules, Solids, Nuclei, and Particles
, John Wiley & Sons
, 2nd
, 59–60
, 978-0-471-87373-0
, For both large and small wavelengths, both matter and radiation have both particle and wave aspects. [...] But the wave aspects of their motion become more difficult to observe as their wavelengths become shorter. [...] For ordinary macroscopic particles the mass is so large that the momentum is always sufficiently large to make the de Broglie wavelength small enough to be beyond the range of experimental detection, and classical mechanics reigns supreme.
Interactions between particles have been scrutinized for many centuries, and a few simple laws underpin how particles behave in collisions and interactions. The most fundamental of these are the laws of conservation of energy and conservation of momentum, which let us make calculations of particle interactions on scales of magnitude that range from stars to quarks.Isaac Newton (1687). Newton's Laws of Motion (Philosophiae Naturalis Principia Mathematica) These are the prerequisite basics of Newtonian mechanics, a series of statements and equations in Philosophiae Naturalis Principia Mathematica, originally published in 1687.

Dividing an atom

The negatively charged electron has a mass equal to {{frac|1837 or 1836}} of that of a hydrogen atom. The remainder of the hydrogen atom's mass comes from the positively charged proton. The atomic number of an element is the number of protons in its nucleus. Neutrons are neutral particles having a mass slightly greater than that of the proton. Different isotopes of the same element contain the same number of protons but differing numbers of neutrons. The mass number of an isotope is the total number of nucleons (neutrons and protons collectively).Chemistry concerns itself with how electron sharing binds atoms into structures such as crystals and molecules. Nuclear physics deals with how protons and neutrons arrange themselves in nuclei. The study of subatomic particles, atoms and molecules, and their structure and interactions, requires quantum mechanics. Analyzing processes that change the numbers and types of particles requires quantum field theory. The study of subatomic particles per se is called particle physics. The term high-energy physics is nearly synonymous to "particle physics" since creation of particles requires high energies: it occurs only as a result of cosmic rays, or in particle accelerators. Particle phenomenology systematizes the knowledge about subatomic particles obtained from these experiments.Taiebyzadeh, Payam (2017). String Theory; A unified theory and inner dimension of elementary particles (BazDahm). Riverside, Iran: Shamloo Publications Center. {{ISBN|978-600-116-684-6}}.


The term "subatomic particle" is largely a retronym of the 1960s, used to distinguish a large number of baryons and mesons (which comprise hadrons) from particles that are now thought to be truly elementary. Before that hadrons were usually classified as "elementary" because their composition was unknown.A list of important discoveries follows:{| class="wikitable"
|Electron {{subatomic particle|electron}}
|elementary (lepton)
|G. Johnstone Stoney (1874)
|J. J. Thomson (1897)
|Minimum unit of electrical charge, for which Stoney suggested the name in 1891.
JOURNAL, Klemperer, Otto, 1959, Electron physics: The physics of the free electron, Physics Today, 13, 6, 64–66, 1960PhT....13R..64K, 10.1063/1.3057011,
|alpha particle {{subatomic particle|alpha}}
|composite (atomic nucleus)
|Ernest Rutherford (1899)
|Proven by Rutherford and Thomas Royds in 1907 to be helium nuclei.
|Photon {{subatomic particle|photon}}
|elementary (quantum)
|Max Planck (1900) {{nobreak|Albert Einstein}} (1905)
|Ernest Rutherford (1899) as γ rays
|Necessary to solve the thermodynamic problem of black-body radiation.
|Proton {{subatomic particle|proton}}
|composite (baryon)
|long ago
|Ernest Rutherford (1919, named 1920)
|The nucleus of {{SimpleNuclide2|hydrogen|1|link=yes}}.
|Neutron {{subatomic particle|neutron}}
|composite (baryon)
|Ernest Rutherford ({{circa}}1918)
|James Chadwick (1932)
|The second nucleon.

|Paul Dirac (1928)
|Carl D. Anderson ({{subatomic particle|positron|link=yes}}, 1932)
|Revised explanation uses CPT symmetry.
|Pions {{subatomic particle|pion}}
|composite (mesons)
|Hideki Yukawa (1935)
|César Lattes, Giuseppe Occhialini (1947) and Cecil Powell
|Explains the nuclear force between nucleons. The first meson (by modern definition) to be discovered.
|Muon {{subatomic particle|muon}}
|elementary (lepton)
|Carl D. Anderson (1936)
|Called a "meson" at first; but today classed as a lepton.
|Kaons {{subatomic particle|kaon}}
|composite (mesons)
|Discovered in cosmic rays. The first strange particle.
|Lambda baryons {{subatomic particle|Lambda}}
|composite (baryons)
|University of Melbourne ({{subatomic particle|Lambda0}}, 1950)Some sources such as WEB,weblink The Strange Quark, indicate 1947.
|The first hyperon discovered.
|Neutrino {{subatomic particle|neutrino}}
|elementary (lepton)
|Wolfgang Pauli (1930), named by Enrico Fermi
|Clyde Cowan, Frederick Reines ({{subatomic particle|electron neutrino|link=yes}}, 1956)
|Solved the problem of energy spectrum of beta decay.
|Quarks({{subatomic particle|up quark}}, {{subatomic particle|down quark}}, {{subatomic particle|strange quark}})
|Murray Gell-Mann, George Zweig (1964)
| colspan=2 |No particular confirmation event for the quark model.
|charm quark {{subatomic particle|charm quark}}
|elementary (quark)
|bottom quark {{subatomic particle|bottom quark}}
|elementary (quark)
|Weak gauge bosons
|elementary (quantum)
|Glashow, Weinberg, Salam (1968)
|CERN (1983)
|Properties verified through the 1990s.
|top quark {{subatomic particle|top quark}}
|elementary (quark)
|Does not hadronize, but is necessary to complete the Standard Model.
|Higgs boson
|elementary (quantum)
|Peter Higgs et al. (1964)
|CERN (2012)
|Thought to be confirmed in 2013. More evidence found in 2014.WEB,weblink CERN experiments report new Higgs boson measurements,, 23 June 2014,
| ?
|Zc(3900), 2013, yet to be confirmed as a tetraquark
|A new class of hadrons.
| ?
| colspan=2 |Yet another class of hadrons. {{As of|2019}} several are thought to exist.
|elementary (quantum)
|Albert Einstein (1916)
|Interpretation of a gravitational wave as particles is controversial.
|Magnetic monopole
|elementary (unclassified)
|Paul Dirac (1931)

See also

{{cmn|colwidth=20em| }}



Further reading

General readers
  • Feynman, R.P. & Weinberg, S. (1987). Elementary Particles and the Laws of Physics: The 1986 Dirac Memorial Lectures. Cambridge Univ. Press.
  • BOOK, Brian Greene, Brian Greene, The Elegant Universe, W.W. Norton & Company, 1999, 978-0-393-05858-1, The Elegant Universe,
  • Oerter, Robert (2006). The Theory of Almost Everything: The Standard Model, the Unsung Triumph of Modern Physics. Plume.
  • Schumm, Bruce A. (2004). Deep Down Things: The Breathtaking Beauty of Particle Physics. Johns Hopkins University Press. {{ISBN|0-8018-7971-X}}.
  • BOOK, Martinus Veltman, Martinus Veltman, Facts and Mysteries in Elementary Particle Physics, World Scientific, 2003, 978-981-238-149-1,

  • Coughlan, G.D., J.E. Dodd, and B.M. Gripaios (2006). The Ideas of Particle Physics: An Introduction for Scientists, 3rd ed. Cambridge Univ. Press. An undergraduate text for those not majoring in physics.
  • BOOK, Griffiths, David J., Introduction to Elementary Particles, John Wiley & Sons, 1987, 978-0-471-60386-3,
  • BOOK, Kane, Gordon L., Modern Elementary Particle Physics, Perseus Books, 1987, 978-0-201-11749-3,

External links


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