Elliptic master integrals and the one-loop cosmological wavefunctionLoop corrections to the cosmological wavefunction involve similar integrals to those required for scattering amplitudes. For the one-loop triangle of a conformally coupled scalar, the master…Amara McCune, Matthew D. Schwartz·Oct 28, 2026SaveLearn
Collective Bootstrap for Matrix Quantum MechanicsWe develop a collective bootstrap framework for large N matrix quantum mechanics formulated directly in the loop space of single trace coordinate moments. Loop joining and splitting operations…Xianlong Liu·Oct 28, 2026SaveLearn
Unifying energy-entropy bounds in semiclassical gravityWe revisit bounds on energy and entropy in semiclassical gravity, aiming to strengthen and unify established bounds, in particular the quantum focussing conjecture (QFC) and the smeared null energy…Jackson R. Fliss, Andrew Rolph·Oct 28, 2026SaveLearn
The Effective Field Theory Origin of the Fuzzy Sphere MethodFuzzy sphere Hamiltonians for (2+1)D conformal field theories are usually written directly on the lowest Landau level. We introduce a framework organizing them as descendants of local ``mother…Mykola Dedushenko·Oct 28, 2026SaveLearn
Topological interfaces between universes and generalized families of 2d QFTsTwo-dimensional quantum field theories with topological point operators decompose into universes. Just as fusion categories have played an important role in understanding non-invertible symmetries,…Pinak Banerjee, Yuhan Gai, Alonso Perez-Lona et al.·Oct 28, 2026SaveLearn
Bootstrapping Wilson lines in Critical Bosonic QED3 Part 1: Large-N endpoint correlators and CFT dataWe study the conformal Wilson line with general charge q in critical bosonic QED3 with N complex scalar flavors by combining diagrammatic four-point calculations with endpoint crossing. We…Jun Maeda, Toshiki Onagi, Soichiro Shimamori·Oct 28, 2026SaveLearn
Conformal Spectrum of (Super) Chiral Ising and XY ModelsWe determine the spectrum of scaling dimensions of composite operators in the critical Gross-Neveu-Yukawa and Nambu-Jona-Lasinio-Yukawa models through a next-to-leading order semiclassical…Oleg Antipin, Jahmall Bersini, Jacob Hafjall et al.·Oct 28, 2026SaveLearn
The Non-Relativistic Limit of Five-Dimensional Boson Stars and Scale Invariance ViolationWe investigate the non-relativistic limit of spherically symmetric boson stars in (4+1)-dimensional general relativity (GR). In this limit, the resulting Newtonian theory exhibits an exact scale…Eduard Kim, Oleg Kondrashov, Emin Nugaev et al.·Oct 28, 2026SaveLearn
Resurgence and Modularity in the First Painlevé EquationFor the first Painlevé equation, we relate three nonlinear Stokes maps associated with a full turn around infinity to modular transformations of the two-parameter tau function through the identity…Kohei Iwaki, Noam Tamarin·Oct 28, 2026SaveLearn
The Topological String on the Quintic to Genus 83 and the Rank-Two D4-D2-D0 IndicesWe compute quintic Gopakumar-Vafa invariants for genera 2-83 and degrees up to 44 by integrating the holomorphic anomaly equations. Under rank-one modularity for the required Gieseker invariants and…Michael Hecht·Oct 28, 2026SaveLearn
Tachyon and massless sectors of the bosonic string effective actionRecently, it has been observed that in certain schemes of the bosonic string effective action, the non-derivative tachyon appears only in the tachyon potential, while all other couplings involve…Mohammad R. Garousi·Oct 28, 2026SaveLearn
Circuit complexity of coupled four-mode squeezed states in two-field inflationWe study the circuit complexity of coupled curvature and entropy perturbations in two-field inflation. We start from the quadratic action and derive the full Hamiltonian. The Hamiltonian includes all…Tao Li, Hai-Bing Fu, Lei-Hua Liu·Oct 28, 2026SaveLearn
Entropically favored scalar hair on AdS black branesWe construct neutral AdS5 black branes with source-free scalar hair that is entropically favored over the symmetric phase. A quadratic scalar--Gauss--Bonnet coupling destabilizes the thermal state…Alex Buchel·Oct 28, 2026SaveLearn
Covering Surfaces, Conical-Defect Continuation, and Multi-Entropy at Arbitrary GenusWe derive normalized geometric factors for permutation-twist correlators at arbitrary genus. For three uniformly ramified branch values, hypergeometric uniformization shows that the real part of the…Chen-Te Ma·Oct 28, 2026SaveLearn
Quotient Quiver Subtraction -- Product GroupsQuotient quiver subtraction translates the gauging of Coulomb branch global symmetries into a combinatoric operation on 3d N=4 gauge theories. This work uses brane systems to introduce a…Sam Bennett, Amihay Hanany, Guhesh Kumaran·Oct 27, 2026SaveLearn
Near-horizon BF bounds for the t+ KK tower on extremal AdS5 black holesWe study the charged Breitenlohner--Freedman (BF) bound for all horizon harmonics of the type IIB t+ Kaluza--Klein tower on extremal charged AdS5 black holes with equal rotations. The scalar…Xiao-Long Liu, Zheng Miao, Yuezhang Tang·Oct 27, 2026SaveLearn
Differential Equations for Dressed "in-in" CorrelatorsWe extend the formalism of differential equations and Integration-by-Parts identities, to cosmological in-in correlators of conformally coupled scalar fields, that can be formulated as dressed flat…Ivo Sachs·Oct 27, 2026SaveLearn
Go with the flow(s): radial de Sitter holography and T2 (+ Λ2)What can we learn about a putative dual to de Sitter spacetime from the bulk? Conversely, what can a candidate dual theory teach us about the bulk? In this work, we construct midisuperspace…Matthew J. Blacker·Oct 27, 2026SaveLearn
Quiver Lab -- A Computing Tool for Quiver Gauge TheoriesQuiver Lab is a browser-based workspace for drawing quivers and exploring the moduli spaces of three-dimensional N = 4 theories. It computes Higgs and Coulomb branch Hilbert series,…Zhenghao Zhong·Oct 27, 2026SaveLearn
Holomorphic fermions in AdS2On two-dimensional Anti-de Sitter space, Majorana fermions with a discrete set of finely tuned, non-zero mass parameters possess conserved spinor--tensors that are symmetric and traceless. In complex…Calvin Y. -R. Chen, Lukas W. Lindwasser·Oct 27, 2026SaveLearn
Black Hole Entropy from Entangled Quantum Reference FramesIn the extended phase space of Donnelly and Freidel, the edge modes of a Schwarzschild black hole are dynamical reference frames whose phase space is the cotangent bundle of…Ludovic Varrin·Oct 27, 2026SaveLearn
Creation of the Universe in Lorentzian Classical GravityThe singularity theorems and the past incompleteness of inflationary spacetimes suggest that the beginning of the Universe lies beyond the domain of semiclassical gravity. We show that the creation…Avipsa Chakrabarti, Avik Chakraborty, Martín Molina et al.·Oct 27, 2026SaveLearn
The 't Hooft model on (A)dS2We solve large-N two-dimensional QCD with fundamental quarks---the 't Hooft model---on rigid AdS2 and dS2. Their isometries preserve the null gauge A-=0 and in affine coordinates the…Panos Betzios·Oct 27, 2026SaveLearn
Stability of Axion--SU(2) Chromomagnetic Condensates with Stochastic Spin-2 DressingWe investigate whether a stochastic spin-2 gauge-field background can stabilize the chromomagnetic condensate of axion--SU(2) Yang--Mills theory at fixed axion Noether charge in flat spacetime. By…Sha Azyzy, Azadeh Maleknejad, Vahid Kamali·Oct 27, 2026SaveLearn
A Spin on Radiation Reaction with CutsWe derive the radiation-reaction equations of motion for a spinning charged body, the Kerr particle, through quadratic order in its spin, generalising the Abraham--Lorentz--Dirac…Asaad Elkhidir, Matteo Sergola, Pablo Vives Matasan·Oct 27, 2026SaveLearn