Skip to content
DraconiticResearch
Search Sources API
186,125 studies31 sourcesUpdated 23 min ago
PreprintarXiv licencearXiv

Five-dimensional Geometry from Spinning Amplitudes

Abstract

Massive spinor-helicity variables in four dimensions are a useful tool for studying amplitudes between higher-spin fields and gravitons. Among them a special, simple set of amplitudes reproduces the linearized stress-energy tensor of a Kerr black hole in the classical limit. In this work we initiate the study of the classical limit of three-point spinor-helicity amplitudes in five dimensions. We introduce the map between the spinor invariants and the expectation values of spin operators and match the amplitude building blocks with those of the multipole expansion. Interestingly, in order to take the classical limit of a general amplitude, we need to augment the multipole structures with the Hodge dual of the classical spin tensor. We study the classical limit of alternative spinning states not described by fully-symmetric products of polarisations and conclude that they can describe the same spacetimes. Finally, by relaxing the orthogonality condition of the spin tensor we are able to model spacetimes with a single rotational isometry and match these to the classical limit of amplitudes allowing for an internal spin shift. Along the way we also identify the class of amplitudes describing the Myers-Perry black hole and comment on its generalization to arbitrary dimensions.

Related

  1. Transverse geometry reshapes current and tracer fluctuation amplitudes in quasi-one-dimensional single files
    Olivier Bénichou, Aurélien Grabsch
    Reports on Progress in PhysicsPeer-reviewedCC BY 4.0Full textCondensed matterStatistical & nonlinear physicsHALarXiv
  2. Big Bounce, Big Crunch Cycle: Gauge Geometry, Full Vector Coupling, and Observational Signatures of a Five-Dimensional Bessel--Klein--Gordon Framework, Paper II of a two-part series
    Jacek Wolejszo
    HALPreprintPublisher termsFull textGeneral earth scienceGeneral physicsHAL
  3. An Amplitudes Approach to Spinning Black Hole Scattering
    Dogan Akpinar
    arXivPreprintCC BY 4.0Full textGravitation & general relativityHigh-energy & particle physicsarXiv
  4. Exact spinning wormholes in five dimensions from Toda integrability
    Masato Nozawa
    arXivPreprintarXiv licenceFull textGravitation & general relativityHigh-energy & particle physicsarXiv
  5. Descartes Curvature Geometry, Compact-Cycle Amplitudes, and the GST Cabibbo Seed
    Andrew M. Brilliant
    arXivPreprintCC BY-NC-ND 4.0Full textGeneral physicsarXiv
BibTeX
@misc{cangemi2026fivedimensional,
  title = {{Five-dimensional Geometry from Spinning Amplitudes}},
  author = {Lucile Cangemi and Iustin Surubaru},
  howpublished = {arXiv},
  year = {2026},
  month = aug,
  doi = {10.48550/arxiv.2605.29831},
  eprint = {2605.29831},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2605.29831},
}
RIS
TY  - UNPB
TI  - Five-dimensional Geometry from Spinning Amplitudes
AU  - Lucile Cangemi
AU  - Iustin Surubaru
PY  - 2026
DA  - 2026/08/28
PB  - arXiv
DO  - 10.48550/arxiv.2605.29831
UR  - https://arxiv.org/abs/2605.29831
AB  - Massive spinor-helicity variables in four dimensions are a useful tool for studying amplitudes between higher-spin fields and gravitons. Among them a special, simple set of amplitudes reproduces the linearized stress-energy tensor of a Kerr black hole in the classical limit. In this work we initiate the study of the classical limit of three-point spinor-helicity amplitudes in five dimensions. We introduce the map between the spinor invariants and the expectation values of spin operators and match the amplitude building blocks with those of the multipole expansion. Interestingly, in order to take the classical limit of a general amplitude, we need to augment the multipole structures with the Hodge dual of the classical spin tensor. We study the classical limit of alternative spinning states not described by fully-symmetric products of polarisations and conclude that they can describe the same spacetimes. Finally, by relaxing the orthogonality condition of the spin tensor we are able to model spacetimes with a single rotational isometry and match these to the classical limit of amplitudes allowing for an internal spin shift. Along the way we also identify the class of amplitudes describing the Myers-Perry black hole and comment on its generalization to arbitrary dimensions.
ER  -