Search arXivSearch

arXiv · 2609.10432

Null String Holography, Null Strings Probe Projective Boundary of Their Target Spaces

Abstract

We prove that the \textit{minimal null string theory} on background manifold ${\cal M}$ is classically equivalent to the ILST theory on the projective boundary of $\mathcal M$, ${\mathcal B}_{_{\text{P}}}={\partial_{_{\text{P}}}\mathcal{M}}$. We conjecture that this equivalence also holds as quantum level, which we dub \textit{null string holography}. In particular, we show classical null string theory on Poincaré patch of $D$ dimensional Anti de Sitter (AdS$_D$) background is described by ILST on $D-1$ dimensional Minkowski background, paralleling the celebrated AdS/CFT. Null strings on cosmological patch of dS$_D$ is governed by ILST on $D-1$ dimensional flat Euclidean space. For null strings on $D$ dimensional Minkowski space, depending on the coordinate patch used, the projective boundary where the ``dual'' ILST theory resides, can by dS$_{D-1}$, $D-1$ dimensional Carrollian space and $D-1$ dimensional hyperboloid, respectively including spacelike asymptotic boundary $ι^0$, asymptotic null boundaries ${\cal I}^\pm$ and timelike infinities $ι^\pm$. We comment on physical implications of the null string holography on black hole backgrounds whose projective boundary includes horizons.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

M. M. Sheikh-Jabbari, H. Yavartanoo. 2026-09-09. Null String Holography, Null Strings Probe Projective Boundary of Their Target Spaces. https://arxiv.org/abs/2609.10432

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

Gaillard-Zumino non-invertible symmetries

We uncover an infinite class of novel zero-form non-invertible symmetries in a broad family of four-dimensional models, studied years ago by Gaillard and Zumino (GZ), which includes several extended supergravities as particular subcases. The GZ models consist of abelian gauge fields coupled to a neutral sector, typically including a set of scalars, whose equations of motion are classically invariant under a continuous group $\mathscr{G}$ acting on the electric and magnetic field strengths via symplectic transformations. The standard lore holds that, at the quantum level, these symmetries are broken to an integral subgroup $\mathscr{G}_\mathbb{Z}$. We show that, in fact, a much larger subgroup $\mathscr{G}_\mathbb{Q}$ survives, albeit through non-invertible topological defects. We explicitly construct these defects and compute some of their fusion rules. As illustrative examples, we consider the axion-dilaton-Maxwell model and the bosonic sector of a class of $\mathcal{N}=2$ supergravities of the kind that appear in type II Calabi-Yau compactifications. Finally, we comment on how (part of) these non-invertible zero-form symmetries can be broken by gauging the $\mathscr{G}_\mathbb{Z}$ subgroup of invertible symmetries.

hep-th

On the resolution of categorical symmetries in (Non-) Unitary Rational CFTs

We explore several aspects of categorical symmetry-resolved entanglement entropy (SREE) directly within two-dimensional rational conformal field theory (RCFT) (without invoking any SymTFT construction arXiv:2409.02806). We derive a general formula applicable whenever the action of the relevant topological defect lines on the annulus Hilbert space is known. This framework accommodates weakly and strongly symmetric boundaries, cloaking states, and fusion rings with multiplicities. We verify the formula in a range of diagonal unitary and non-unitary examples, including theories with generalized Haagerup-Izumi modular data. Furthermore, we extend the analysis to non-diagonal RCFTs. The $\frac{1}{2}E_6$ example demonstrates that closed-channel modular data and NIM-rep multiplicities alone do not suffice to determine the defect action on the complete open-channel Hilbert space.

hep-th

Reflecting boundary conditions in critical loop models

In critical loop models, we call a boundary sticky if loops can attach to it, and reflecting otherwise. Using analytic bootstrap methods, we show that reflecting boundaries are characterised by one complex parameter, analogous to the boundary cosmological constant in Liouville theory. We determine disc 1-point functions, and write an explicit formula for disc 2-point functions as infinite combinations of conformal blocks. We also sketch the lattice interpretation of reflecting boundaries.

hep-th