
doi: 10.1007/bf02733552
The role of the gauge invariance is analysed. Such an invariance guarantees that the given vector field (of electromagnetic or Yang-Mills kind) describes spin 1 only. Contrary to the statement of many authors (1–13) it is shown that the requirement of the gauge invariance cannot be a principle for obtaining nontrivial interactions and for deducing the existence of any vector field.
quantum theory
quantum theory
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