Skip to content
DraconiticResearch
Search Sources API
186,125 studies31 sourcesUpdated 35 min ago
PreprintarXiv licencearXiv

Tensionless limit of M5-brane and conformal symmetry of its bosonic body

Abstract

We obtain a tensionless limit of the M-theory 5-brane action and discuss its properties. The consistency of this limit requires that the field strength H3 of the 2-form gauge field on the M5 brane worldvolume is non-vanishing and non-degenerate, so that one can also regard it as a strong H3-field limit. The induced 6d worldvolume metric of this theory is non-degenerate in contrast to conventional tensionless (null) p-branes. We find that the tensionless M5-brane action is invariant under a super-Weyl symmetry acting on the bulk supergeometry, while in the purely bosonic case the action is invariant under an 11D target-space conformal symmetry, a property which is characteristic for the tensionless bosonic branes. Upon imposing a static gauge, which fixes worldvolume diffeomorphisms, this 11D conformal symmetry becomes a deformed 6d worldvolume conformal symmetry whose action on the worldvolume coordinates involves field dependent terms. When the transversal fluctuations of the 5-brane in the bulk are zero, the model reduces to the conformal non-linear chiral 2-form electrodynamics considered earlier by Gibbons and West, and by Townsend.

Related

  1. Dynamical classical-field limit of Bosonic Gibbs states: Renormalized Hartree NLS correlations in 2D and 3D
    Phan Thành Nam, Rongchan Zhu, Xiangchan Zhu
    arXivPreprintarXiv licenceFull textAnalysis & PDEsMathematical physicsarXiv
  2. Exact SU(N) symmetry resolution of bosonic Hubbard models: general boson-fermion mappings and flat-band singlet-cluster states
    Loïc Herviou
    HALPreprintCC BY-NC 4.0Full textMathematical physicsAtomic, molecular & optical physicsHALarXiv
  3. New time-periodic solutions to the cubic conformal wave equation on 𝕊3: I Spherical symmetry
    Filip Ficek, Maciej Maliborski
    arXivPreprintarXiv licenceFull textAnalysis & PDEsMathematical physicsarXiv
  4. JT gravity as a conformal scaling limit of random flat combinatorial disks
    Morris Ang
    arXivPreprintCC BY 4.0Full textMathematical physicsProbabilityarXiv
  5. Dear Quantizers, Stochastic ≈ Brane
    Justin Kulp
    arXivPreprintarXiv licenceFull textMathematical physicsHigh-energy & particle physicsarXiv
BibTeX
@misc{bandos2026tensionless,
  title = {{Tensionless limit of M5-brane and conformal symmetry of its bosonic body}},
  author = {Igor Bandos and Kurt Lechner and Dmitri P. Sorokin},
  howpublished = {arXiv},
  year = {2026},
  month = sep,
  doi = {10.48550/arxiv.2607.29653},
  eprint = {2607.29653},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2607.29653},
}
RIS
TY  - UNPB
TI  - Tensionless limit of M5-brane and conformal symmetry of its bosonic body
AU  - Igor Bandos
AU  - Kurt Lechner
AU  - Dmitri P. Sorokin
PY  - 2026
DA  - 2026/09/24
PB  - arXiv
DO  - 10.48550/arxiv.2607.29653
UR  - https://arxiv.org/abs/2607.29653
AB  - We obtain a tensionless limit of the M-theory 5-brane action and discuss its properties. The consistency of this limit requires that the field strength H_3 of the 2-form gauge field on the M5 brane worldvolume is non-vanishing and non-degenerate, so that one can also regard it as a strong H_3-field limit. The induced 6d worldvolume metric of this theory is non-degenerate in contrast to conventional tensionless (null) p-branes. We find that the tensionless M5-brane action is invariant under a super-Weyl symmetry acting on the bulk supergeometry, while in the purely bosonic case the action is invariant under an 11D target-space conformal symmetry, a property which is characteristic for the tensionless bosonic branes. Upon imposing a static gauge, which fixes worldvolume diffeomorphisms, this 11D conformal symmetry becomes a deformed 6d worldvolume conformal symmetry whose action on the worldvolume coordinates involves field dependent terms. When the transversal fluctuations of the 5-brane in the bulk are zero, the model reduces to the conformal non-linear chiral 2-form electrodynamics considered earlier by Gibbons and West, and by Townsend.
ER  -