Free geometric equations for higher spins
By D. Francia, A. Sagnotti. 2002
237 citations recorded by the source corpus.
Abstract We show how allowing non-local terms in the field equations of symmetric tensors uncovers a neat geometry that naturally generalizes the Maxwell and Einstein cases. The end results can be related to multiple traces of the generalized Riemann curvatures R α 1 ⋯α s ;β 1 ⋯β s introduced by de Wit and Freedman, divided by suitable powers of the D'Alembertian operator □. The conventional local equations can be recovered by a partial gauge fixing involving the trace of the gauge parameters Λα1⋯αs−1, absent in the Fronsdal formulation. The same geometry underlies the fermionic equations, that, for all spins s+1/2, can be linked via the operator ∂ □ to those of the spin-s bosons.
Subfields: Applied Mathematics, Atomic and Molecular Physics, and Optics, Statistical and Nonlinear Physics
View Paper: https://www.semanticscholar.org/paper/f501ff84653f64728904bec101493ba75f0d0b74
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In Applied Mathematics
In Atomic and Molecular Physics, and Optics
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Citations in the corpus
- Unfolding mixed-symmetry fields in AdS and the BMV conjecture: I. General formalism (2008, methodology): “, B, B = B, h J = h J for J 6= I, I +1 , and h I = h I −1 , (13)Totally symmetric sl(D)-tensor gauge fields were first considered in [44] though the dynamical field equation was not of the form (4.”
- Cubic interactions of massless higher spins in (A)dS: Metric-like approach (2011, background): “See [34–37] for other recent developments in the frame-like approach to the cubic-interaction problem.”
- An Introduction to free higher-spin fields (2004, methodology): “In this section we show how one can obtain very simple local non-Lagrangian descriptions that exhibit the unconstrained gauge symmetry present in the non-local equations and reduce to the Fronsdal form after a partial gauge fixing [3, 4, 5].”
- Effective action in a higher-spin background (2010, background): “odes can be misleading. Moreover, imposing from the beginning trace constraints on the higher-spin fields would break the non-Abelian symmetry group of unitary operators. The unconstrained formulation [41] and the triplets [42] both rely on unconstrained higher-spin tensors but the local actions invo”