E and J type N=(0,2) disordered models and higher-spin symmetryIn this work, we investigate the emergence of higher-spin structure in 2d N=(0,2) disordered models. While previous studies focused on the J-type model where the E-term in the Fermi…Liang Wang, Miao Wang·Jul 13, 2026SaveLearn
Extracting light-cone wave functions from covariant amplitudes: a detailed study in scalar field theoryWe propose a conjectured formula that systematically maps covariant off-shell amplitudes to light-cone wave functions in scalar field theory. Through an explicit comparison at one-loop accuracy, we…Stéphane Munier·Jul 13, 2026SaveLearn
Resonance phenomena in vortex-antivortex collisionsIn this work, we provide a full map of scattering scenarios between a Nielsen-Olesen vortex and antivortex. Importantly, in the deep type II regime, such a collision reveals a chaotic pattern in the…Maximilian Bachmaier, Andrzej Wereszczynski·Jul 13, 2026SaveLearn
Tensor Reduction of Sunset by Generating FunctionRecently, the generating function has been proposed as an alternative reduction method. This method has been tested at the one-loop level, including the tensor reduction and propagators with higher…Xinhe Chen, Bo Feng, Liang Zhang·Jul 13, 2026SaveLearn
SymTFT for Continuous Symmetries: Non-linear Realizations and Spontaneous BreakingIt is well known that continuous symmetries of quantum fields can be realized non-linearly, e.g. in the context of sigma models, and can also be spontaneously broken on non-compact spacetimes. In…Federico Bonetti, Michele Del Zotto, Ruben Minasian·Jul 13, 2026SaveLearn
Accelerating Universe from ConstraintsWe introduce a framework of constrained scalar fields that can give rise to cosmological evolution of the Universe independent of the values of the cosmological constant. Focusing on the simplest…Anamaria Hell, Misao Sasaki·Jul 13, 2026SaveLearn
The tricritical Ising CFT and conformal bootstrapThe tricritical Ising CFT is the IR fixed-point of λϕ6 theory. It can be seen as a one-parameter family of CFTs connecting between an -expansion near the upper critical dimension 3…Johan Henriksson·Jul 13, 2026SaveLearn
Krylov Complexity from Loschmidt AmplitudeKrylov complexity is a powerful diagnostic of quantum dynamics, with clear connections to other measures of quantum chaos and operator growth. One such measure is the Loschmidt amplitude, defined as…Debarghya Chakraborty·Jul 12, 2026SaveLearn
The Euler-Heisenberg action for a U(1)× U(1) dyon quantum electrodynamicsThe one-loop effective Lagrangian of quantum electrodynamics for dyons (dQED) with a U(1) × U(1) gauge symmetry is derived using the Schwinger proper-time method. We identify the analog of the…D. O. R. Azevedo, T. S. Dias, E. D. Pereira·Jul 12, 2026SaveLearn
Certified boundary-magic witness for state-dependent proto-area in a holographic codeWe study a four-qubit product-EPR holographic code whose reconstructing region contains matter and one leg of a geometry bond. Seven deformations compare local, bipartite, bond-stabilizing, and…Luis Lozano·Jul 12, 2026SaveLearn
Deformed BTZ Radiance and Single Trace TT HolographyWe generalize the "holar wind" mechanism proposed in arXiv:2303.00234 to the case of rotating λ-deformed BTZ black holes. These backgrounds, which interpolate between AdS3 in the…Daniel Vainshtein·Jul 12, 2026SaveLearn
Weyl Anomaly Coefficients of Holographic Defect CFTs at Weak and Strong CouplingWe determine the type-A Weyl anomaly coefficient b, associated with the intrinsic scalar curvature of the defect, for the class of holographically realised co-dimension two defect CFTs (dCFTs)…George Georgiou·Jul 12, 2026SaveLearn
Quantum Vacuum energy as the origin of GravityWe explore the idea that quantum vacuum energy ρ vac is at the origin of Gravity. We formulate a gravitational version of the electromagnetic Casimir effect, and provide an argument for how…André LeClair·Jul 12, 2026SaveLearn
D-branes in AdS2 × H2 × H2 under the non-Abelian T-dualityWe proceed to construct a non-Abelian dual pair for the AdS2 × H2 × H2 background by applying the non-Abelian T-duality (here as Poisson-Lie T-duality on a semi-Abelian double). By…Ali Eghbali·Jul 11, 2026SaveLearn
Superspace invariants and 3-point correlators in 3d N=3,4 SCFTsWe use the auxiliary polarization spinor formalism together with superspace techniques to construct a complete and minimal list of 3-point invariant structures in three-dimensional superconformal…Aditya Jain, Amin A. Nizami·Jul 11, 2026SaveLearn
Meson states in `t Hooft model: Hamiltonian approachWe point out that the masses of the highly excited bound quark-antiquark states in QCD2 in the infinite N limit may be determined in the framework of a simple quantum-mechanical model with the…A. V. Smilga·Jul 11, 2026SaveLearn
Self-Gravitating Magnetic Monopoles and Dyons in String-Inspired Models: Structure and StabilityWe present classical magnetic--monopole (MM) and dyon solutions induced by global monopoles in string-inspired gravitational models. Although several ingredients of the construction have appeared…Nick E. Mavromatos, Sarben Sarkar, Dionysios P. Theodosopoulos·Jul 11, 2026SaveLearn
The many facets of a hyperbolic tetrahedron: open and closed triangulations of 3d gravityWe study a model of 3d gravity relevant to the open sector of a CFT ensemble. The quantum theory is the open Virasoro TQFT, obtained by restricting the full open-closed Virasoro TQFT to a subclass of…Daniel L. Jafferis, Diandian Wang·Jul 11, 2026SaveLearn
Spectral Curves with Complex Multiplication in Hermitian Matrix ModelsWe show that elliptic curves with complex multiplication (CM) naturally emerge in the spectral geometry of Hermitian one-matrix models in the two-cut phase. Focusing on a symmetric quartic potential,…Ali Nassar·Jul 11, 2026SaveLearn
Anomaly cancellation for two U(1) factorsWe show that solving the abelian part of the local anomaly cancellation conditions for a 4-d gauge theory whose gauge Lie algebra has an abelian summand with rank K ≥ 1 is equivalent to the…Ben Gripaios, Khoi Le Nguyen Nguyen·Jul 10, 2026SaveLearn
Spinning the Large-Charge Bootstrap: Parity-Even OperatorsWe study the large-charge bootstrap in three-dimensional CFTs with a global U(1) symmetry using scalar, current, and stress-tensor probes, restricting to parity-even exchanged operators. Under…Kasra Kiaee, Alexander Monin·Jul 10, 2026SaveLearn
Perusing confining pseudoreal theories: a story of emerging massless spin-1 bosonsSolving quantum field theory, which is at the basis of the standard model of particle interactions, is one of the main tasks of contemporary theoretical physics. Minimal asymptotically free…Giacomo Cacciapaglia, Konstantinos Kollias·Jul 10, 2026SaveLearn
Monodromy and geometry of heavy-light Virasoro blocksThe AdS/CFT correspondence relates gravity in anti-de Sitter space to a boundary conformal field theory, and in its AdS3/CFT2 instance the Virasoro symmetry of the boundary theory organizes…Mikhail Belakovskiy, Vladimir Belavin·Jul 10, 2026SaveLearn
Factorization Algebras and Quantum Groups from Generalized Poisson Sigma ModelsIn this work we introduce and study a family of holomorphic--topological field theories, which we call generalized Poisson sigma models. These theories are higher-dimensional analogues of the…Keyou Zeng·Jul 10, 2026SaveLearn
Unified description of color-electric and color-magnetic strings in hybrid vacua of N=2 supersymmetric QCDWe study non-Abelian strings supported in r-vacua of 4D N=2 supersymmetric QCD (SQCD) with gauge group U(N) and Nf quark hypermultiplets (Nf N), where r<N (scalar) quarks…E. Ievlev, D. Vasilev, A. Yung·Jul 10, 2026SaveLearn