Dirac fermion
In physics, a Dirac fermion is spin 1⁄2 particle (a fermion) which is different from its antiparticle. The vast majority of fermions – perhaps all – fall under this category.
Description
In particle physics all fermions in the standard model have distinct antiparticles (perhaps excepting neutrinos) and hence are Dirac fermions. They are named for Paul Dirac, and can be modeled with the Dirac equation.
A Dirac fermion is equivalent to two Weyl fermions.[1] The counterpart to a Dirac fermion is a Majorana fermion, a particle that must be its own antiparticle.
Dirac fermion quasi-particles
In condensed matter physics, low-energy excitations in graphene and topological insulators, among others, are fermionic quasiparticles described by a pseudo-relativistic Dirac equation.
gollark: It should be available in `_G.json` anyway.
gollark: The JSON one in the ROM SHOULD mostly work.
gollark: Also, what would your ”bank” actually do?
gollark: Or you need to mine correctly.
gollark: Another partial fix would be to encode the number of loops or whatever in metadata and to use that, but that would be hacky.
See also
- Dirac spinor, a wavefunction-like description of a Dirac fermion
- Majorana fermion, an alternate category of fermion, possibly describing neutrinos
- Spinor, mathematical details
References
- Shifman, Mikhail (1999). "ITEP Lectures on Particle Physics and Field Theory". 1: 292. ISBN 9789810239480. Cite journal requires
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