Subatomic Particle
A subatomic particle is a particle that is smaller (but not necessarily lighter) than an atom . Particle physics and nuclear physics are primarily concerned with subatomic particles . The subatomic particles can be divided into elementary particles and composite particles .
The subatomic particles were extensively studied in the 20th century . Due to the variety of discovered particles, the so-called particle zoo was sometimes referred to . It was only through the concept of quarks that it was possible to understand the internal structure of the hadrons. The development culminated in the standard model that has existed for almost 50 years .
Due to their quantum nature , subatomic particles cannot be thought of as classical particles. Rather, quantum phenomena such as wave-particle dualism , uncertainty relations , vacuum fluctuations and virtual particles appear in the physical description of the behavior and reactions of subatomic particles .
Types of subatomic particles
Elementary particles
A distinction is made between the confirmed elementary particles of the Standard Model:
- Quarks
- Leptons
- Calibration bosons
- as well as the Higgs boson
Compound particles
With the composite particles the situation is more complicated. The composite particles that have subatomic dimensions are all made up of combinations of quark elementary particles. The quarks themselves cannot be observed or measured alone, only their decay products. One differentiates:
-
Hadrons :
- Mesons : quark-antiquark pairs
- Baryons : 3 quarks. This also includes the nucleons protons and neutrons
- Exotic hadrons: tetraquarks and pentaquarks
- other composite particles:
At the atomic level, i.e. above the subatomic level, there are not only ordinary atoms and molecules, but also so-called exotic atoms , which are created by combining subatomic hadrons and other elementary particles. An example of an exotic atom is muonic hydrogen .
Well-known examples
- Elementary particles: photon , electron
- Composed: protons , neutrons , alpha particles or, in general, atomic nuclei
Fermions and bosons
Another important distinction between subatomic particles is that between fermions and bosons . These classes differ in two basic properties:
- In every quantum state of a system, e.g. B. of an atom, there is only at most one fermion of a given type (see Pauli principle ); this restriction does not apply to bosons. This difference is described by the fact that different probability distributions apply for fermions and bosons, the Fermi-Dirac statistics and the Bose-Einstein statistics . The spin of a particle is linked to the statistics via the spin statistics theorem . Thus, fermions and bosons also differ in their half- integer and integer spin quantum numbers.
- The elementary fermions, i.e. leptons and quarks, can only be created or destroyed together with an antiparticle. This observation, which explains the stability of matter, is described by the law of conservation of the number of particles ( baryon number , lepton number ). Elementary bosons, on the other hand, can arise and perish individually.
All components of the atom, proton, neutron and electron, are fermions. Only the Pauli principle makes the structure of atomic nuclei and the electron shells understandable. The elementary particles are also mostly fermions. Only the gauge bosons (including the photon) and the Higgs particle are bosons. Among the composite particles, the mesons belong to the bosons.
Important phenomena at the subatomic level
- radioactivity
- Nuclear fusion
- Photoelectric effect
- Stability of the atomic nucleus: the mass of the atomic nucleus is mainly created by the binding energy of the quarks.
Major discoveries of subatomic particles
Subatomic Particle | composition | Theoretical concept | Discovered experimentally | Comments |
---|---|---|---|---|
electron | elemental ( lepton ) | 1874: G. Johnstone Stoney | 1897: JJ Thomson | Minimum unit for the electrical charge, which is why Stoney proposed this name in 1891. |
Alpha particles | composite (atomic nucleus) | - | 1899: Ernest Rutherford | In 1907 it was confirmed by Rutherford and Thomas Royds that they were helium nuclei |
photon | elementary ( gauge boson ) | 1900: Max Planck | 1905: Albert Einstein or Ernest Rutherford (1899) as gamma radiation |
Necessary to understand the black body problem of thermodynamics . |
proton | compound ( baryon ) | - | 1919: Ernest Rutherford | The nucleus of the hydrogen atom and the first nucleon of the atomic nuclei |
neutron | compound ( baryon ) | 1918, possibly as early as 1917: Ernest Rutherford | 1932: James Chadwick | The second nucleon of the atomic nucleus. |
positron | elemental ( antilepton ) | 1928: Paul Dirac | 1932: Carl D. Anderson | Antiparticle of the electron, first evidence of antimatter |
Pion | compound ( meson ) | 1935: Hideki Yukawa | 1947: César Lattes , Giuseppe Occhialini and Cecil Powell | Pion exchange model describes forces in the atomic nucleus |
Muon | elemental (lepton) | - | 1936: Carl D. Anderson | - |
Kaon | compound (meson) | - | 1947 | Discovered in cosmic rays . The first particle with a strange quark . |
Lambda baryon | compound (baryon) | - | 1950, possibly even 1947: University of Melbourne | The first one discovered Hyperon |
neutrino | elemental (lepton) | 1930: Wolfgang Pauli , named by Enrico Fermi | 1956: Clyde Cowan , Frederick Reines | Necessary to understand the energy spectrum during beta decay. |
Quarks (up, down, strange) |
elementary | 1964: Murray Gell-Mann , George Zweig | - | Confirmed indirectly because this model explains the particle zoo |
Charm quark | elementary (quark) | 1970 | 1974: Both by Burton Richter et al. at the Stanford Linear Accelerator Center , as well as Samuel Chao Chung Ting et al. at Brookhaven National Laboratory . (1974) | Part of the J / ψ meson |
Bottom curd | elementary (quark) | 1973 | 1977: Fermilab , group led by Leon Max Lederman | Part of the Υ meson |
W bosons and Z boson | elementary (gauge boson) | 1968: Glass show , Weinberg , Salam | 1983: CERN | Properties confirmed in the 1990s |
Top curd | elementary (quark) | 1973 | 1995 | Lifetime is too short to be able to be detected directly in a hadron |
Higgs boson | elementary | 1964: Peter Higgs et al. | 2012: CERN | Confirmed since 2014 at the latest |
See also
literature
- RP Feynman and S. Weinberg : Elementary Particles and the Laws of Physics: The 1986 Dirac Memorial Lectures . Cambridge University Press, 1987.
- Brian Greene: The Elegant Universe . WW Norton & Company, 1999, ISBN 0-393-05858-1 .
- Robert Oerter: The Theory of Almost Everything: The Standard Model, the Unsung Triumph of Modern Physics . Plume, 2006.
- Bruce A. Schumm: Deep Down Things: The Breathtaking Beauty of Particle Physics . Johns Hopkins University Press, 2004, ISBN 0-8018-7971-X . .
- Martinus Veltman: Facts and Mysteries in Elementary Particle Physics . World Scientific, 2003, ISBN 981-238-149-X .
- GD Coughlan, JE Dodd and BM Gripaios: The Ideas of Particle Physics: An Introduction for Scientists. 3rd edition, Cambridge University Press, 2006. An undergraduate text for those not majoring in physics.
- David J. Griffiths: Introduction to Elementary Particles . Wiley, John & Sons, Inc., 1987, ISBN 0-471-60386-4 .
- Gordon L. Kane: Modern Elementary Particle Physics . Perseus Books, 1987, ISBN 0-201-11749-5 .
Individual evidence
- ^ Otto Klemperer: Electron Physics: The Physics of the Free Electron . Academic Press , 1959.
- ^ The Strange Quark
- ↑ SLAC-SP-017 Collaboration (JE Augustin et al.): Discovery of a Narrow Resonance in e + e - Annihilation. In: Physical Review Letters. Volume 33, 1974, pp. 1406-1408 ( online )
- ↑ E598 Collaboration (JJ Aubert et al.): Experimental Observation Of A Heavy Particle J. In: Physical Review Letters. Volume 33, 1974, pp. 1404-1406 ( online )
- ↑ CERN experiments report new Higgs boson measurements . cern.ch (June 23, 2014)