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| Format: | Preprint |
| Published: |
2024
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| Subjects: | |
| Online Access: | https://arxiv.org/abs/2412.20557 |
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| _version_ | 1866912172137775104 |
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| author | Sazdovic, Branislav |
| author_facet | Sazdovic, Branislav |
| contents | In previous two articles we postulated that field equations for arbitrary spin and helicity are Casimir eigenvalue equations. In massive case, from such principle equation, we derived spin-$0$ Klein-Gordon, spin-$\frac{1}{2}$ Dirac and spin-$1$ vector equations. In the present article we will derived spin-$\frac{3}{2}$ Rarita-Schwinger equation, which is nontrivial combination of vector and spinor case. We will also show that vector-spinor field contains two spin-$\frac{1}{2}$ Dirac fields. |
| format | Preprint |
| id |
arxiv_https___arxiv_org_abs_2412_20557 |
| institution | arXiv |
| publishDate | 2024 |
| record_format | arxiv |
| spellingShingle | Rarita-Schwinger equation from principle equation for all spins Sazdovic, Branislav High Energy Physics - Theory In previous two articles we postulated that field equations for arbitrary spin and helicity are Casimir eigenvalue equations. In massive case, from such principle equation, we derived spin-$0$ Klein-Gordon, spin-$\frac{1}{2}$ Dirac and spin-$1$ vector equations. In the present article we will derived spin-$\frac{3}{2}$ Rarita-Schwinger equation, which is nontrivial combination of vector and spinor case. We will also show that vector-spinor field contains two spin-$\frac{1}{2}$ Dirac fields. |
| title | Rarita-Schwinger equation from principle equation for all spins |
| topic | High Energy Physics - Theory |
| url | https://arxiv.org/abs/2412.20557 |