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In particle physics, the Dirac equation is a relativistic wave equation derived by British physicist Paul Dirac in 1928. In its free form, or including electromagnetic interactions, it describes all spin-.mw-parser-output .sfrac{white-space:nowrap}.mw-parser-output .sfrac.tion,.mw-parser-output .sfrac…
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equation dirac displaystyle quantum spinor field theory representation also matrices symmetry group relativistic form lorentz spin vector mechanics spinors action
| Subject | Predicate | Object | Confidence | Src |
|---|---|---|---|---|
| Dirac equation | is a | relativistic wave equation derived by British physicist Paul Dirac in 1928 | 0.90 | text |
| Dirac equation | is a | relativistic analogue of the Schrödinger equation for the Dirac fermion wavefunction.In the second quantization form of quantum field theory the Dirac spinor is quantized to be… | 0.90 | text |
| Dirac equation | is a | Lorentz covariant equation | 0.90 | text |
| Dirac equation | is a | similar multi-body equation.A geometric reformulation of the Dirac equation is known as the Dirac | 0.90 | text |
| atomic nuclei | instance of | the scattering of electrons off a heavy target | 0.80 | text |
| followed the next year | instance of | the scattering of electrons off a heavy target | 0.80 | text |
| Moller scattering in 1932 | instance of | Over the following years it was further used to derive other standard scattering processes | 0.80 | text |
| Bhabha scattering in 1936.A problem that gained more focus with time was the presence of negative energy states in the Dirac equation | instance of | Over the following years it was further used to derive other standard scattering processes | 0.80 | text |
| which led to many efforts to try to eliminate such states | instance of | Over the following years it was further used to derive other standard scattering processes | 0.80 | text |
| anomalies | instance of | this may not always be possible in the full quantum theory due to various obstructions | 0.80 | text |
| which signal that the full quantum theory is not invariant under the local symmetry despite its classical Lagrangian being invariant | instance of | this may not always be possible in the full quantum theory due to various obstructions | 0.80 | text |
| Dirac equation | related to Consequences | Except | 0.60 | section |
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