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Gravitational Couplings of Higher Spins from String Theory
High Energy Physics - Theory · Submitted 30 May 2010
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim This is consistent with the general structure of the non-Abelian $2-s-s$ couplings, implying that the minimal number of space-time derivatives in the interaction vertices of two spin s and one spin 2 particle is equal to $2s-2$.
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The abstract, sentence by sentence
We calculate the interaction 3-vertex of two massless spin 3 particles with a graviton using vertex operators for spin 3 fields in open string theory, constructed in our previous work. The massless spin 3 fields are shown to interact with the graviton through the linearized Weyl tensor, reproducing the result by Boulanger, Leclercq and Sundell. This is consistent with the general structure of the non-Abelian $2-s-s$ couplings, implying that the minimal number of space-time derivatives in the interaction vertices of two spin s and one spin 2 particle is equal to $2s-2$.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We calculate the interaction 3-vertex of two massless spin 3 particles with a graviton using vertex operators for spin 3 fields in open string theory, constructed in our previous work. | contribution 0.87 | 0.94 | 0.08 | asserted 1.00 |
| s1 | The massless spin 3 fields are shown to interact with the graviton through the linearized Weyl tensor, reproducing the result by Boulanger, Leclercq and Sundell. | result 0.99 | 0.84 | 0.32 | asserted 1.00 |
| s2 | This is consistent with the general structure of the non-Abelian $2-s-s$ couplings, implying that the minimal number of space-time derivatives in the interaction vertices of two spin s and one spin 2 particle is equal to $2s-2$. | interpretation 0.99 | 0.45 | 0.60 | hedged possibility 0.53 |
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The paper
Original abstract
We calculate the interaction 3-vertex of two massless spin 3 particles with a graviton using vertex operators for spin 3 fields in open string theory, constructed in our previous work. The massless spin 3 fields are shown to interact with the graviton through the linearized Weyl tensor, reproducing the result by Boulanger, Leclercq and Sundell. This is consistent with the general structure of the non-Abelian $2-s-s$ couplings, implying that the minimal number of space-time derivatives in the interaction vertices of two spin s and one spin 2 particle is equal to $2s-2$.
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References
How the literature uses it
19 arXiv papers cite this in 21 sentences
Papers citing it · 13 sentences without a confident label
Cites it as background 8 papers
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The results [ref] and [ref] concern higher-spin gauge fields which, when described in the metric-like or Fronsdal formalism [ref] , are given by totally symmetric rank-$s$ tensors[For recent works on cubic couplings among totally symmetric fields see [ref] .].
Gravitational cubic interactions for a simple mixed-symmetry gauge field in AdS and flat backgrounds · Introduction · 0.96
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A preliminary step towards this goal would be to construct the most general consistent cubic couplings.[ Many efforts have been devoted in this direction: see the references in [ref] for an exhaustive list of works, and in particular the latest works [ref] and [ref] for flat-space and (A)dS interactions involving totally-symmetric HS fields, respectively.] Among them, only a subset is expected to be compatible with higher-order interactions [ref] and lead eventually to fully non-linear theories.
Generating functions of (partially-)massless higher-spin cubic interactions · Introduction · 0.95
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One can observe during the last years growing interest in this topic connected with recent progress in the construction of cubic interactions for higher spin gauge fields and its association to string theory [ref] - [ref] , which gave new insights in earlier important works [ref] - [ref] .
Radial Reduction and Cubic Interaction for Higher Spins in (A)dS space · Introduction · 0.81
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