Resurgence and Riemann--Hilbert problems for orientifolded conifoldsWe study the crosscap part of the large-N SO/Sp orientifold conifold free energies. The unprojected crosscap block is a single q-Pochhammer tower. Its rank-one shift equation matches the…Wu-yen Chuang, Yi-Jing Tseng·Jun 5, 2026SaveLearn
Gravitationally Induced UV Completion of an O(N) Scalar TheoryWe investigate the ultraviolet completion of an O(N) scalar field theory non-minimally coupled to gravity using the Wilsonian functional renormalization group in the proper-time formulation.…Alfio M. Bonanno, Emiliano M. Glaviano·Jun 5, 2026SaveLearn
Amplifying the Cosmological Collider with Ghost SpectatorsGhost inflation is a well-known framework in which cosmological fluctuations can generate enhanced primordial non-Gaussianity, typically of the equilateral type. In its original form, however, it is…Matheus Curado Ferreira, F. T. Falciano, Guilherme L. Pimentel·Jun 5, 2026SaveLearn
Black Hole States in Quantum Spin ChainsWe define a black hole state in a spin chain by studying thermal correlators in holography. Focusing on the Heisenberg model we investigate the thermal and complexity properties of the black hole…Charlotte Kristjansen, Konstantin Zarembo·Jun 5, 2026SaveLearn
Induced energy-momentum tensor of the scalar field in 3D de Sitter QEDIn this work, we derive the renormalized expectation value of the energy--momentum tensor of a quantized charged scalar field in three-dimensional de Sitter spacetime dS3 in the…Manizheh Botshekananfard, Takahiro Hayashinaka·Jun 5, 2026SaveLearn
Holography of K-complexity: Switchbacks and ShockwavesIn this paper we study Krylov complexity in the presence of single and multiple operators in the DSSYK model, where we can use the analytical techniques coming from chord diagrammatics. One of the…Marco Ambrosini, Eliezer Rabinovici, Julian Sonner·Jun 5, 2026SaveLearn
Linear Resistivity from Spatially Random Interactions and the Uniqueness of Yukawa CouplingRecent studies have shown that a spatially random Yukawa-type interaction between a Fermi surface and critical bosons can produce linear-in-temperature resistivity, the defining signature of strange…Sang-Jin Sin, Yi-Li Wang·Jun 5, 2026SaveLearn
Carroll Geometry Meets De Sitter Space via HolographyWe explain how to relate the ideas of Carroll geometry, matrix theory on instantonic objects, and infinite boost limits of M-theory. Based on these new insights, we explore the implications for…Chris D. A. Blair, Niels A. Obers, Ziqi Yan·Jun 5, 2026SaveLearn
Quantum-corrected black hole thermodynamics from the gravitational path integralExploring quantum effects from black hole thermodynamics has always been a pivotal topic. In recent years, the free energy landscape and ensemble-averaged theory based on the Euclidean path integral…Yu-Qi Liu, Hao-Wei Yu, Peng Cheng·Jun 5, 2026SaveLearn
Holographic CFT Thermodynamics as a Bridge Between the Weak Gravity and Weak Cosmic Censorship Conjectures for EMPYM--AdS Black HolesThe weak cosmic censorship conjecture () and the weak gravity conjecture () sit at the heart of how singularities and charged matter are constrained in any consistent theory of quantum…Saeed Noori Gashti, Behnam Pourhassan, Izzet Sakalli et al.·Jun 4, 2026SaveLearn
Finite N Black Holes through the Brick WallIn AdS/CFT at finite N, black holes are described by ordinary quantum systems with finite entropy and discrete spectra, while semiclassical bulk effective field theory treats the near-horizon region…Seiji Terashima·Jun 4, 2026SaveLearn
Instanton-Induced Closed-String Amplitudes in Minimal Superstring Theory at Subleading OrderWe compute the disk one-point function, the disk two-point function, and the annulus one-point function of the cosmological constant operator in the type 0A and type 0B minimal superstring theories…Jyotirmoy Barman, Rishabh Kaushik, Raghu Mahajan et al.·Jun 4, 2026SaveLearn
Closing the loop on Φ4 in AdS3We compute the one-loop correction to the CFT data of all double-trace operators [ϕϕ]n, for a Φ4 theory in AdS3, for arbitrary values of n, , and of the scaling dimension…Dean Carmi, Riccardo Ciccone, Shimon Sukholuski·Jun 4, 2026SaveLearn
Three Advanced Lectures on InflationLecture notes on inflation. The lectures are three double lectures, held for the first time at the Nordita Winter School 2024 - Particle Physics and Cosmology, covering an advanced introduction to…Martin S. Sloth·Jun 4, 2026SaveLearn
Smooth horizons from topology change in canonical quantum gravityWe propose a resolution of the firewall paradox in JT gravity by incorporating topology change into canonical quantization under relational time evolution. The gravitational Hamiltonian acts on the…Venkatesa Chandrasekaran·Jun 4, 2026SaveLearn
Quantum Geometry from Area FluctuationsWe construct a quantum-statistical analogue of Einstein's fluctuation argument for black-body radiation in the context of causal-diamond geometry. Starting from the phase space of a stretched…Jerzy Kowalski-Glikman, Ludovic Varrin·Jun 4, 2026SaveLearn
Spinning bulk-to-boundary correlators in the massless theories with Poincaré symmetryWe classify the bulk-to-boundary correlators for general integer-spin s operators in a Poincaré-invariant theory by imposing suitable fall-off conditions near future/past null infinity. Any…Jiang Long, Yu-Xuan Wei, Xin-Hao Zhou·Jun 4, 2026SaveLearn
A note on the 2D NLSM free energyThis note contains the perturbative computation of the 2D non-linear sigma model (NLSM) energy-density in a chemical potential h, at the fourth order in the coupling constant expansion. The result…Yizhuang Liu·Jun 4, 2026SaveLearn
Chiral symmetry breaking in models with unconventional supersymmetryWe investigate dynamical mass generation in a geometrically constructed gauge theory based on the super Lie algebra su(2,2|3), in which gravity, Yang-Mills fields, and fermions are unified as…Pedro D. Alvarez, Cristian Villavicencio, Jorge Zanelli·Jun 4, 2026SaveLearn
Detecting Topological Transitions and Anisotropy through Multipartite Entanglement in Holographic Weyl SemimetalsWe study multipartite entanglement structures in the zero-temperature holographic Weyl semimetal, focusing on tripartite and four-partite structures. For strip regions, we compute the conditional…Xiantong Chen, Xuanting Ji, Wen-Peng Li et al.·Jun 4, 2026SaveLearn
Charting the different phases of Yang-Mills-Chern-Simons-Higgs theoriesWe explore Yang-Mills-Chern-Simons theories coupled to a Higgs-like field in the fundamental representation of SU(2) quantized in linear covariant gauges in three Euclidean dimensions. We analyze…Daniel O. R. Azevedo, Gustavo P. de Brito, Philipe De Fabritiis et al.·Jun 4, 2026SaveLearn
Fermionic Kaluza-Klein mode mixing in braneworldsWe investigate fermionic Kaluza-Klein (KK) mode mixing in thick braneworld models subjected to generic background perturbations. Conventionally, isolated static backgrounds are completely described…Chun-E Fu, Wen-Xuan Ma·Jun 4, 2026SaveLearn
AdS9 solutions in type II supergravitiesWe present new solutions in type II supergravities describing AdS9 geometries warped over an interval. In type IIB, we construct an analytic family of backgrounds supported by a non-trivial…Giuseppe Dibitetto, Nicolò Petri·Jun 4, 2026SaveLearn
AdSD× I solutions in axio-dilaton gravityWe study non-supersymmetric AdSD× I solutions in the context of (D+1) dimensional gravity coupled to an axio-dilaton with arbitrary runaway potential for the dilaton and arbitrary…Giuseppe Dibitetto, Nicolò Petri·Jun 4, 2026SaveLearn
The Awada-Gibbons-Shaw Algebra in de Sitter Space and SUSY BreakingWe rederive the Cosmological Supersymmetry Breaking Relation m3/2 = CRdS LP from a deformation of the Awada-Gibbons-Shaw local supersymmetry algebra.T. Banks·Jun 4, 2026SaveLearn