Physics:Quantum fermion: Difference between revisions
Remove hidden BOM characters and set Book II after Short description |
Remove hidden BOM characters and direct Book label after Short description |
||
| Line 3: | Line 3: | ||
{{Short description|Half-integer-spin quantum particle obeying Fermi-Dirac statistics}} | {{Short description|Half-integer-spin quantum particle obeying Fermi-Dirac statistics}}I | ||
{{Quantum matter backlink|Particles}} | {{Quantum matter backlink|Particles}} | ||
Revision as of 11:05, 22 May 2026
I
fermion is a Book II topic in the Quantum Collection. A quantum fermion is a particle with half-integer spin that obeys Fermi-Dirac statistics. Fermions have antisymmetric many-particle wavefunctions, so identical fermions cannot occupy the same one-particle quantum state. This rule gives matter much of its structure, from atomic shells to degenerate stars. A quantum fermion is a particle with half-integer spin that obeys Fermi-Dirac statistics. Fermions have antisymmetric many-particle wavefunctions, so identical fermions cannot occupy the same one-particle quantum state. This rule gives matter much of its structure, from atomic shells to degenerate stars. The spin-statistics connection links half-integer spin with fermionic exchange behavior in relativistic quantum theory. Exchanging two identical fermions changes the sign of the many-body wavefunction.
Spin and statistics
The spin-statistics connection links half-integer spin with fermionic exchange behavior in relativistic quantum theory. Exchanging two identical fermions changes the sign of the many-body wavefunction. The resulting Pauli exclusion principle is not an ordinary force; it is a constraint on the allowed quantum states.[1]
Elementary and composite fermions
Elementary fermions include quarks and leptons. Composite systems can also behave as fermions when their total spin is half-integer, as in protons, neutrons, many nuclei, atoms, and quasiparticle excitations in condensed matter.
Physical consequences
Fermion statistics explain the periodic structure of atoms, electron degeneracy pressure, band filling in solids, and the stability of ordinary matter. In particle physics, fermion flavor, chirality, and mass mixing are central to weak interactions, neutrino oscillations, and matter-antimatter studies.[2]
Description
fermion is a matter-scale concept used to organize how quantum theory describes atoms, particles, fields, condensed matter, plasma, or spacetime-related systems. In the Quantum Collection it is placed by scale so the reader can move from materials and molecules down to subatomic degrees of freedom.
Quantum context
At this scale, the relevant behavior is controlled by quantized states, interactions, conservation laws, and the way excitations or particles are observed. The concept is normally linked to measurable properties such as energy, momentum, charge, spin, spectra, scattering rates, or collective modes.
Role in the collection
This page provides a compact reference point for related pages in Book II. It should be read together with nearby matter-scale topics and the corresponding foundations in quantum mechanics.[3]
See also
Table of contents (84 articles)
Index
Full contents
References
- ↑ Peskin, Michael E.; Schroeder, Daniel V. (1995). An Introduction to Quantum Field Theory. Addison-Wesley. ISBN 978-0-201-50397-5.
- ↑ Griffiths, David J. (2008). Introduction to Elementary Particles (2nd ed.). Wiley-VCH. ISBN 978-3-527-40601-2.
- ↑ "Quantum mechanics". https://en.wikipedia.org/wiki/Quantum_mechanics.
Source attribution: Physics:Quantum fermion
