Supersymmetric spectroscopy on \( \mathrm{AdS}_4 \times S^7\) and \( \mathrm{AdS}_4 \times S^6\)
From MaRDI portal
Publication:1981479
DOI10.1007/JHEP07(2021)094zbMath1468.83056arXiv2103.13408MaRDI QIDQ1981479
Oscar Varela, Gabriel Larios, Mattia Cesàro
Publication date: 3 September 2021
Published in: Journal of High Energy Physics (Search for Journal in Brave)
Full work available at URL: https://arxiv.org/abs/2103.13408
Supergravity (83E50) Supersymmetric field theories in quantum mechanics (81T60) Infinite-dimensional groups and algebras motivated by physics, including Virasoro, Kac-Moody, (W)-algebras and other current algebras and their representations (81R10) Kaluza-Klein and other higher-dimensional theories (83E15)
Related Items (9)
On the superconformal index of Chern-Simons theories and their KK spectrometry ⋮ Holographic 3d \(\mathcal{N} = 1\) conformal manifolds ⋮ Consistent truncations in higher derivative supergravity ⋮ \( \mathcal{N} = 1\) S-fold spectroscopy ⋮ On generalised D1-D5 near horizons and their spectra ⋮ Kaluza-Klein spectrometry beyond consistent truncations: the squashed \(S^7\) ⋮ On the squashed seven-sphere operator spectrum ⋮ The spectrum of marginally-deformed \(\mathcal{N} = 2\) CFTs with \(\mathrm{AdS}_4\) S-fold duals of type IIB ⋮ Triality and the consistent reductions on \(\mathrm{AdS}_3 \times S^3\)
Uses Software
Cites Work
- Supersymmetric \(E_{7(7)}\) exceptional field theory
- \({\mathcal N=2}\) supersymmetric \(\mathrm{AdS}_4\) solutions of M-theory
- \(M\)-theory, exceptional generalised geometry and superpotentials
- Generalized geometry and M theory
- Spin-2 spectrum of defect theories
- \(N=8\) supergravity with local scaling symmetry
- General \(\mathcal N=1\) supersymmetric fluxes in massive type IIA string theory
- The maximal \(D=5\) supergravities
- Classification of supersymmetric flux vacua in M-theory
- AdS/CFT correspondence and symmetry breaking
- M-theory on \(\text{AdS}_4\times M^{111}\): The complete \(\text{Osp}(2|4) \times \text{SU}(3) \times \text{SU}(2)\) spectrum from harmonic analysis
- A massive class of \( \mathcal{N}=2 \) \(\mathrm{AdS}_{4}\) IIA solutions
- Dyonic \(\mathrm{ISO}(7)\) supergravity and the duality hierarchy
- \(\mathrm{AdS}_{4}\) solutions of massive IIA from dyonic \(\mathrm{ISO}(7)\) supergravity
- Exceptional generalised geometry for massive IIA and consistent reductions
- The exceptional story of massive IIA supergravity
- Spectrum universality properties of holographic Chern-Simons theories
- An \(\mathrm{SO}(3)\times\mathrm{SO}(3)\) invariant solution of \(D = 11\) supergravity
- The geometry of \( \mathcal{N}=3 \) \(\mathrm{AdS}_{4}\) in massive IIA
- All homogeneous \(N=2\) M-theory truncations with supersymmetric AdS\(_4\) vacua
- All \(G_2\) invariant critical points of maximal supergravity
- Branes at conical singularities and holography
- New \(\mathrm{AdS}_4\) vacua in dyonic ISO(7) gauged supergravity
- Kaluza-Klein fermion mass matrices from exceptional field theory and \(\mathcal{N} = 1\) spectra
- Kaluza-Klein spectroscopy for the Leigh-Strassler SCFT
- Super-Chern-Simons spectra from exceptional field theory
- Universal properties of Kaluza-Klein gravitons
- Flowing to \(\mathcal{N} = 3\) Chern-Simons-matter theory
- Tachyonic Kaluza-Klein modes and the AdS swampland conjecture
- Fourteen new stationary points in the scalar potential of SO(8)-gauged \(\mathcal{N} = 8\), \(D = 4\) supergravity
- SO(8) supergravity and the magic of machine learning
- The role of singletons in \(S^7\) compactifications
- Gauged supergravities
- Consistent \( \mathcal{N}=8 \) truncation of massive IIA on \(S^{6}\)
- A cubic deformation of ABJM: the squashed, stretched, warped, and perturbed gets invaded
- Supergravity in theory in 11 dimensions
- The structure of \({\mathcal N}=3\) multiplets in \(\text{AdS}_4\) and the complete \(\text{OSp}(3|4)\times\text{SU}(3)\) spectrum of M-theory on \(\text{AdS}_4\times N^{0,1,0}\)
- An \(N=2\) supersymmetric membrane flow
This page was built for publication: Supersymmetric spectroscopy on \( \mathrm{AdS}_4 \times S^7\) and \( \mathrm{AdS}_4 \times S^6\)
