Localisation with on-shell supersymmetry algebras via the Batalin-Vilkovisky formalism: Localisation as gauge fixingThe Batalin-Vilkovisky formalism provides a powerful technique to deal with gauge and global (super)symmetries that may only hold on shell. We argue that, since global (super)symmetries and gauge…Leron Borsten, Dimitri Kanakaris, Hyungrok Kim·Nov 3, 2025SaveLearn
2D or not 2D: a "holographic dictionary" for Lowest Landau LevelsWe consider 2D fermions on a plane with a perpendicular magnetic field, described by Landau levels. It is wellknown that, semiclassically, restriction to the lowest Landau levels (LLL) implies two…Gautam Mandal, Ajay Mohan, Rushikesh Suroshe·Nov 3, 2025SaveLearn
On the phase of the de Sitter density of statesThe one-loop gravitational path integral around Euclidean de Sitter space SD has a complex phase that casts doubt on a state counting interpretation. Recently, it was proposed to cancel this phase…Yiming Chen, Douglas Stanford, Haifeng Tang et al.·Nov 3, 2025SaveLearn
Emergent Area Operators in the BoundaryIn some cases in two and three bulk dimensions without bulk local degrees of freedom, I look for area operators in a fixed boundary theory. In each case, I define an exact quantum error-correcting…Ronak M Soni·Nov 3, 2025SaveLearn
8D conformal gravity with Einstein sector, and its relation to the Q-curvatureWe first streamline the construction of the unique six-dimensional conformal gravity action found by Lü, Pang and Pope, that admits Einstein metrics as solutions to the field equations. We then prove…Nicolas Boulanger, Davide Rovere·Nov 3, 2025SaveLearn
Symmetry-Resolved Entanglement Entropy from Heat KernelsWe develop a systematic framework for computing symmetry-resolved entanglement entropies (SREE) in charged quantum systems based on an improved heat kernel approach. Although the conventional…Yuan-Chun Jing, Chao Niu, Zhuo-Yu Xian·Nov 3, 2025SaveLearn
Thermal Bootstrap of Large-N Matrix Models via Conic OptimizationThis paper is aimed at improving thermal bootstrapping methods for matrix quantum mechanics. The thermal energies of the large-N one-matrix anharmonic oscillator and large-N two-matrix anharmonic…Sophia Adams·Nov 3, 2025SaveLearn
Translation invariant defects as an extension of topological symmetriesThe modern way to understand symmetries of a quantum field theory is via its topological defects in various dimensions. In this contribution to the proceedings we focus on line defects in 2d QFT and…Federico Ambrosino, Ingo Runkel, Gérard M. T. Watts·Nov 3, 2025SaveLearn
Near-extremal membranes in M-theoryWe consider near-extremal membranes embedded in M-theory, consistently truncated to gauged N = 2 supergravity in four dimensions on the coset space M1,1,0. These are holographically…Alex Buchel, Ruben Monten·Nov 3, 2025SaveLearn
Entanglement asymmetry in gauge theories: chiral anomaly in the finite temperature massless Schwinger modelThe entanglement asymmetry has emerged in recent years as a practical quantity to study phases of matter. We present the first study of entanglement asymmetry in gauge theories by considering the…Adrien Florio, Sara Murciano·Nov 3, 2025SaveLearn
Effervescent Spikes in M-theoryAdS3 × S3 × S3 solutions warped over a Riemann surface, Σ, are indexed by a parameter, γ, that defines the superconformal algebra, D(2,1; γ) D(2,1; γ) they preserve.…Iosif Bena, Raphaël Dulac, Dimitrios Toulikas et al.·Nov 3, 2025SaveLearn
Symmetries and dualities in non-supersymmetric CHL stringsWe chart the classical moduli space of heterotic strings with broken supersymmetry a la Scherk-Schwarz and gauge group rank reduced by 8 in eight dimensions. This space consists of four connected…Bernardo Fraiman, Héctor Parra de Freitas·Nov 3, 2025SaveLearn
Wiggling boundary and corner edge modes in JT gravity with defectsWe study the gravitational edge modes (GrEMs) and gauge edge modes (GaEMs) in Jackiw-Teitelboim (JT) gravity on a wiggling boundary. The wiggling effect manifests as a series of spacetime topological…Kang Liu, Shoupan Liu, Xiao-Mei Kuang·Nov 3, 2025SaveLearn
Black holes and dualities in string theory compactificationsThis thesis addresses three problems arising in type II string theory compactified on a Calabi-Yau manifold. In the first one we study the hypermultiplet moduli space (HM), by working on its twistor…Khalil Bendriss·Nov 2, 2025SaveLearn
Symmetry-resolved genuine multi-entropy: Haar random and graph statesWe study the symmetry-resolved genuine multi-entropy, a measure that captures genuine multi-partite entanglement, in Haar random states and random graph states in the presence of a conserved…Norihiro Iizuka, Simon Lin·Nov 2, 2025SaveLearn
Black hole interiors of homogeneous holographic solids under shear strainWe investigate the interior of AdS black holes under finite shear strain in a class of holographic axion models, which are widely used to describe strongly-coupled systems with broken translations.…Yuanceng Xu, Li Li, Wei-Jia Li·Nov 2, 2025SaveLearn
Fortuity with a single matrixWe construct and study a supersymmetric quantum mechanical model with a single U(N) adjoint fermionic matrix. The model is exactly solvable yet contains a large number of fortuitous states. We…Yiming Chen·Nov 2, 2025SaveLearn
Quantum Complexity of Nonlocal Field TheoriesEntanglement entropy for nonlocal field theories displays a universal ``volume law" scaling Barbon:2008ut, Karczmarek:2013xxa, Shiba:2013jja, Pang:2014tpa as opposed to the ``area law"…Mohan sai Balusu, Gaurav Katoch, Sanhita Parihar et al.·Nov 1, 2025SaveLearn
Weyl double copy in Lifshitz spacetimesLifshitz black hole solutions pose particular challenges for reconciling the two main formulations of the classical double copy: the Kerr-Schild double copy and the Weyl double copy. Recent work has…Gokhan Alkac, Mehmet Kemal Gumus, Mehmet Ali Olpak·Nov 1, 2025SaveLearn
AdS3 Quantum Gravity and Finite N Chiral PrimariesString theory on AdS3 × S3 × M4 provides a well-studied realization of AdS3/CFT2 holography, but its non-perturbative structure at finite N 1/GN(3)…Ji Hoon Lee, Wei Li·Nov 1, 2025SaveLearn
Transmission Coefficients from Phantom CurrentsA representative quantity that characterizes the dynamics of conformal interfaces is the transmission coefficient, which is defined through correlation functions of the stress tensor. Typically, this…Yuma Furuta, Yuya Kusuki, Toshiki Onagi·Nov 1, 2025SaveLearn
Nonlocal MechanicsWe introduce a Hamiltonian framework for nonlocal Lagrangian systems without relying on infinite-derivative expansions. Starting from a (trajectory-based) variational principle and a generalized…Carlos Heredia, Josep Llosa·Nov 1, 2025SaveLearn
Every Wrinkle Carries A Memory: An Integro-differential Bootstrap for Features in Cosmological CorrelatorsMotivated by cosmological observations, we push the cosmological bootstrap program beyond the de Sitter invariance lamppost by considering correlators that explicitly break scale invariance, thereby…Sadra Jazayeri, Xi Tong, Yuhang Zhu·Oct 31, 2025SaveLearn
Twists and Gorms and Antifields, oh my!I define topological twists of supersymmetric field theories in the case when the supercharges involved obey an ``open'' algebra. Using the Batalin-Vilkovisky field-antifield formalism, I…Alex S. Arvanitakis·Oct 31, 2025SaveLearn
N=2 Universality at Strong CouplingWe present a detailed analysis of integrated correlators for an N=2 superconformal field theory on a squashed sphere with SU(N) gauge group and fundamental/anti-symmetric matter.…L. De Lillo, Z. Duan, M. Frau et al.·Oct 31, 2025SaveLearn