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In , a subatomic particle is a smaller than an . According to the , a subatomic particle can be either a composite particle, which is composed of other particles (for example, a , like a or a , composed of three ; or a , composed of two ), or an elementary particle, which is not composed of other particles (for example, quarks; or , , and tau particles, which are called ).

(2025). 9780124158016, .
and study these particles and how they interact.
(2025). 9789812561411, . .
Most force-carrying particles like or are called and, although they have quanta of energy, do not have rest mass or discrete diameters (other than pure energy wavelength) and are unlike the former particles that have rest mass and cannot overlap or combine which are called . The W and Z bosons, however, are an exception to this rule and have relatively large rest masses at approximately and respectively.

Experiments show that light could behave like a stream of particles (called ) as well as exhibiting wave-like properties. This led to the concept of wave–particle duality to reflect that quantum-scale behave both like particles and like ; they are occasionally called wavicles to reflect this.

Another concept, the uncertainty principle, states that some of their properties taken together, such as their simultaneous position and , cannot be measured exactly. Interactions of particles in the framework of quantum field theory are understood as creation and annihilation of of corresponding fundamental interactions. This blends particle physics with field theory.

Even among , the exact definition of a particle has diverse descriptions. These professional attempts at the definition of a particle include:

  • A particle is a collapsed wave function
  • A particle is an excitation of a quantum field
  • A particle is an irreducible representation of the Poincaré group
  • A particle is an observed thing

+ Particles in the atom ! Subatomic particle !! Symbol !! Type !! Location in atom !! Charge !! Mass
≈ 1
≈ 1


Classification

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 are:

(2025). 9780521852494, Cambridge University Press. .

All of these have now been discovered through 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 particle and many other elementary particles, but none have been discovered as of 2021.


Hadrons
The word hadron comes from Greek and was introduced in 1962 by . Nearly all composite particles contain multiple quarks (and/or antiquarks) bound together by gluons (with a few exceptions with no quarks, such as and ). Those containing few (≤ 5) quarks (including antiquarks) are called . 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 containing an odd number of quarks (almost always 3), of which the and (the two ) are by far the best known; and the containing an even number of quarks (almost always 2, one quark and one antiquark), of which the and 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 and one , 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 that do (other than the proton and neutron) form .


By statistics
Any subatomic particle, like any particle in the three-dimensional space that obeys the 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 and therefore feel the strong interaction, and the 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 predict additional elementary particles with spin 3/2, but none have been discovered as of 2023.

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, E = mc2. That is, can be expressed in terms of and vice versa. If a particle has a frame of reference in which it lies at rest, then it has a positive 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 ) is heavier than the two lightest flavours of baryons (). It is also certain that any particle with an 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 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 leptons, as well as baryons by either the strong force or weak force (except for the proton). Protons are not known to , although whether they are "truly" stable is unknown, as some very important Grand Unified Theories (GUTs) actually require it. The μ and τ muons, as well as their antiparticles, decay by the weak force. Neutrinos (and antineutrinos) do not decay, but a related phenomenon of neutrino oscillations is thought to exist even in vacuums. The electron and its antiparticle, the , are theoretically stable due to charge conservation unless a lighter particle having of electric charge   e exists (which is unlikely). Its charge is not shown yet.


Other properties
All observable subatomic particles have their electric charge an multiple of the elementary charge. The Standard Model's quarks have "non-integer" electric charges, namely, multiple of   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 , Satyendra Nath Bose, Louis de Broglie, and many others, current scientific theory holds that all particles also have a wave nature.

(2025). 9783540674580, Springer. .
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.
(1985). 9780471873730, John Wiley & Sons. .

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. 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 of about of that of a atom. The remainder of the hydrogen atom's mass comes from the positively charged . The 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 of the same element contain the same number of protons but different numbers of neutrons. The of an isotope is the total number of (neutrons and protons collectively).

concerns itself with how electron sharing binds atoms into structures such as crystals and . The subatomic particles considered important in the understanding of chemistry are the , the , and the . 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 . 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 , or in particle accelerators. Particle phenomenology systematizes the knowledge about subatomic particles obtained from these experiments.

(2025). 9786001166846, Shamloo Publications.


History
The term " subatomic particle" is largely a of the 1960s, used to distinguish a large number of and (which comprise ) 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:

!Particle
!Composition
!Theorized
!Discovered
!Comments
[[electron]]elementary ([[lepton]])G. Johnstone Stoney (1874) J. J. Thomson (1897) Minimum unit of electrical charge, for which Stoney suggested the name in 1891. First subatomic particle to be identified.
[[alpha particle]]composite (atomic nucleus) Ernest Rutherford (1899) Proven by Rutherford and [[Thomas Royds]] in 1907 to be helium nuclei. Rutherford won the Nobel Prize for Chemistry in 1908 for this discovery.
[[photon]]elementary ([[quantum]])[[Max Planck]] (1900) [[Albert Einstein]] (1905) thermodynamics]] problem of black-body radiation.
[[proton]]composite ([[baryon]])William Prout (1815)
(1993). 9780385312110, Delta. .
Ernest Rutherford (1919, named 1920)The nucleus of .
[[neutron]]composite (baryon)Ernest Rutherford (1920)[[James Chadwick]] (1932) The second [[nucleon]].
[[antiparticle]]s [[Paul Dirac]] (1928)Carl D. Anderson (, 1932)Revised explanation uses [[CPT symmetry]].
[[pion]]scomposite ([[meson]]s)[[Hideki Yukawa]] (1935)César Lattes, Giuseppe Occhialini, [[Cecil Powell]] (1947)Explains the [[nuclear force]] between nucleons. The first meson (by modern definition) to be discovered.
[[muon]]elementary (lepton) Carl D. Anderson (1936)Called a "meson" at first; but today classed as a [[lepton]].
tau
elementary ([[lepton]])[[Antonio Zichichi]] (1960)
Martin Lewis Perl (1975)
composite (mesons) George Rochester]], C. C. Butler (1947)Discovered in [[cosmic ray]]s. The first [[strange particle]].
[[lambda baryon]]scomposite (baryons) University of Melbourne (, 1950)Some sources such as indicate 1947.The first [[hyperon]] discovered.
[[neutrino]]elementary (lepton)[[Wolfgang Pauli]] (1930), named by [[Enrico Fermi]][[Clyde Cowan]], [[Frederick Reines]] (, 1956)Solved the problem of energy [[spectrum]] of [[beta decay]].
[[quark]]s
(, , )
elementary[[Murray Gell-Mann]], [[George Zweig]] (1964)colspan=2 particular confirmation event for the [[quark model]].
[[charm quark]]elementary (quark)[[Sheldon Glashow]], [[John Iliopoulos]], [[Luciano Maiani]] (1970)Burton Richter]], S. C. C. Ting (, 1974)
[[bottom quark]]elementary (quark)Makoto Kobayashi, Toshihide Maskawa (1973)Leon M. Lederman (, 1977)
[[gluon]]selementary (quantum)[[Harald Fritzsch]], [[Murray Gell-Mann]] (1972) [[DESY]] (1979)
weak gauge bosons ,elementary (quantum)[[Sheldon Glashow]], [[Steven Weinberg]], [[Abdus Salam]] (1968)
(1968). 9789810216627 .
[[CERN]] (1983)Properties verified through the 1990s.
[[top quark]]elementary (quark)Makoto Kobayashi, Toshihide Maskawa (1973)[[Fermilab]] (1995)hadronization]], but is necessary to complete the Standard Model.
[[Higgs boson]]elementary (quantum)[[Peter Higgs]] (1964)CERN (2012)Only known spin zero elementary particle.
[[tetraquark]]composite Zc(3900), 2013, yet to be confirmed as a tetraquarkA new class of hadrons.
[[pentaquark]]composite Yet another class of hadrons. several are thought to exist.
[[graviton]]elementary (quantum)Albert Einstein (1916) Interpretation of a gravitational wave as particles is controversial.
magnetic monopoleelementary (unclassified)Paul Dirac (1931)


See also
  • (book)
  • (book)
  • Hot spot effect in subatomic physics
  • List of fictional elements, materials, isotopes and atomic particles
  • List of particles
  • Poincaré symmetry


Further reading

General readers


Textbooks
  • (2025). 9780521677752, Cambridge University Press. .
    An undergraduate text for those not majoring in physics.
  • (2025). 9780471603863, Wiley. .
  • (2025). 9781107165083, Cambridge University Press. .


External links

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