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In mathematical physics, the gamma matrices, { γ 0 , γ 1 , γ 2 , γ 3 } , {\displaystyle \ \left\{\gamma ^{0},\gamma ^{1},\gamma ^{2},\gamma ^{3}\right\}\ ,} also called the Dirac matrices, are a set of conventional matrices with specific anticommutation relations that ensure they generate a matrix representation of the Clifford algebra C l 1 , 3 ( R ) .…
Physical structure, Overview & Other representations
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| Subject | Predicate | Object | Confidence | Src |
|---|---|---|---|---|
| Gamma matrices | related to Charge conjugation | The | 0.60 | section |
| Gamma matrices | related to Charge conjugation | This | 0.60 | section |
| Gamma matrices | related to Charge conjugation | Conjugating | 0.60 | section |
| Gamma matrices | related to Chiral representation | Notice | 0.60 | section |
| Gamma matrices | related to Chiral representation | Euclidean Clifford | 0.60 | section |
| Gamma matrices | related to Chiral representation | It | 0.60 | section |
| Gamma matrices | related to Chiral representation | QCD | 0.60 | section |
| Gamma matrices | related to Cl1,3(C) and Cl1,3(R) | The Dirac | 0.60 | section |
| Gamma matrices | related to Cl1,3(C) and Cl1,3(R) | Cl1 | 0.60 | section |
| Gamma matrices | related to Dirac basis | The | 0.60 | section |
| Gamma matrices | related to Dirac basis | Dirac | 0.60 | section |
| Gamma matrices | related to Dirac basis | To | 0.60 | section |
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