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The most general subsidiary conditions of the second kind of the general Gel’fand-Yaglom wave equation based on the representation (1/2,3/2)⊕(-1/2,3/2)⊕(1/2,5/2)⊕(-1/2,5/2)⊕(1/2,3/2) ⊕ (-1/2,3/2) in the presence of an external electromagnetic field

✍ Scribed by C. G. Koutroulos

No coin nor oath required. For personal study only.

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