Current exchanges and unconstrained higher spins
The (Fang–) Fronsdal formulation for free fully symmetric (spinor-) tensors rests on ( γ-) trace constraints on gauge fields and parameters. When these are relaxed, glimpses of the underlying geometry emerge: the field equations extend to non-local expressions involving the higher-spin curvatures, a...
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Published in | Nuclear physics. B Vol. 773; no. 3; pp. 203 - 237 |
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Main Authors | , , |
Format | Journal Article |
Language | English |
Published |
Elsevier B.V
02.07.2007
North-Holland ; Elsevier [1967-....] |
Subjects | |
Online Access | Get full text |
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Summary: | The (Fang–) Fronsdal formulation for free fully symmetric (spinor-) tensors rests on (
γ-) trace constraints on gauge fields and parameters. When these are relaxed, glimpses of the underlying geometry emerge: the field equations extend to non-local expressions involving the higher-spin curvatures, and with only a pair of additional fields an equivalent “minimal” local formulation is also possible. In this paper we complete the discussion of the “minimal” formulation for fully symmetric (spinor-) tensors, constructing one-parameter families of Lagrangians and extending them to
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backgrounds. We then turn on external currents, that in this setting are subject to conventional conservation laws and, by a close scrutiny of current exchanges in the various formulations, we clarify the precise link between the local and non-local versions of the theory. To this end, we first show the equivalence of the constrained and unconstrained local formulations, and then identify a unique set of non-local Lagrangian equations which behave in the same fashion in current exchanges. |
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ISSN: | 0550-3213 1873-1562 |
DOI: | 10.1016/j.nuclphysb.2007.03.021 |