The tt*-structure for the quantum cohomology of complex GrassmannianThe tt*-equation (topological-anti-topological fusion equation) was introduced by S. Cecotti and C. Vafa for describing massive deformation of supersymmetric conformal field theories. B. Dubrovin…Tadashi Udagawa·Oct 16, 2025SaveLearn
Twistor Wilson loops in large-N Yang-Mills theoryIt has been known for many years that, in Yang-Mills theories with N=4,2,2* supersymmetry, certain nontrivial supersymmetric Wilson loops exist with v.e.v. either trivial or computable…Marco Bochicchio, Giacomo Santoni·Oct 16, 2025SaveLearn
Tracking discontinuities in parameter spaceWe develop a geometric framework in Feynman-parameter space to determine constraints on the sequential discontinuities of Feynman integrals. Our method is based on tracking the deformation of the…Ruth Britto, Holmfridur S. Hannesdottir·Oct 15, 2025SaveLearn
Open case for a closed universeWe establish a new no-go theorem for cosmology: spatially flat (k=0) and open (k=-1) Friedmann--Robertson--Walker (FRW) non-static spacetimes cannot be simultaneously nonsingular, geodesically…Nathan L. Burwig, Damien A. Easson·Oct 15, 2025SaveLearn
Diffeomorphism invariant tensor networks for 3d gravityTensor networks prepare states that share many features of states in quantum gravity. However, standard constructions are not diffeomorphism invariant and do not support an algebra of non-commuting…Vijay Balasubramanian, Charlie Cummings·Oct 15, 2025SaveLearn
On the Imaginary Part of the Effective Action in de Sitter Spacetime with Different Regularization SchemesThe imaginary part of the effective action encodes vacuum instability and particle production in the background field. Two standard approaches are commonly used to derive it: the Bogoliubov method…Yu Zhou, Hai-Qing Zhang·Oct 15, 2025SaveLearn
Four-charge static non-extremal black holes in the five-dimensional N=2, STU-W2U supergravityWe construct, for the first time, new static non-extremal five-dimensional black hole solutions (without or with squashed horizons) endowing with four different electric charge parameters in the $D =…Di Wu, Shuang-Qing Wu·Oct 15, 2025SaveLearn
Logarithmic Corrections to Thermodynamics of Accelerating Black HolesAs pointed out in recent research, the near extremal black hole entropy with one-loop effect exhibits universal T behavior at sufficiently low temperature. In this paper, we discuss the…Jianfei Xu·Oct 15, 2025SaveLearn
Chiral Quartic Massive Gravity in Three DimensionsWe study New Massive Gravity (NMG) with Chern-Simons (CS), cubic, and quartic terms under the Compère-Song-Strominger (CSS) boundary conditions. By employing a semi-product of a Virasoro and a U(1)…Seyed Naseh Sajadi, Supakchai Ponglertsakul·Oct 15, 2025SaveLearn
Shadow sectors of gauge theoriesWe show that both abelian and non-abelian gauge theories admit configurations in which the fields behave as if in the presence of static charge densities, or ``shadow charges". These correspond…Loris Del Grosso, David E. Kaplan, Francesco Serra·Oct 15, 2025SaveLearn
De Sitter holographic complexity from Krylov complexity in DSSYKWe utilize the recent connection between the high energy limit of the double-scaled SYK model and two-dimensional de Sitter solutions of sine dilaton gravity to identify the length of a family of…Michal P. Heller, Fabio Ori, Jacopo Papalini et al.·Oct 15, 2025SaveLearn
Subdimensional Disorder and Logarithmic DefectWe study quenched disorder localized on a p-dimensional subspacetime in a d-dimensional conformal field theory. Motivated by the logarithmic behavior often associated with disorder, we introduce…Soichiro Shimamori, Yifan Wang·Oct 15, 2025SaveLearn
Axion-Scalar Systems and Dynamical DistancesWe study the cosmology of axion-scalar pairs, coupled by a hyperbolic field-space metric and with a string-motivated rational scalar potential. Borrowing tools from the theory of dynamical systems,…Thomas W. Grimm, Damian van de Heisteeg, Filippo Revello·Oct 14, 2025SaveLearn
Branes and Antibranes in AdS3: The Impossible States in the CFT GapWe construct a new family of type IIB supergravity solutions corresponding to states of the D1-D5-P-KKm system that carry the same charges and energy as the non-extremal four-charge black hole and…Roberto Emparan, Pierre Heidmann·Oct 14, 2025SaveLearn
Notes on false vacuum decay in quantum Ising modelsThis paper aims to gather together some of the basic ideas behind the theory of false vacuum decay in quantum Ising models, focusing on the application of spin chains as analogue systems to false…Ian G. Moss·Oct 14, 2025SaveLearn
Classification and Birational Equivalence of Dimer Integrable Systems for Reflexive PolygonsBrane tilings are bipartite periodic graphs on the 2-torus and realize a large family of 4d N=1 supersymmetric gauge theories corresponding to toric Calabi-Yau 3-folds. We present a complete…Minsung Kho, Norton Lee, Rak-Kyeong Seong·Oct 14, 2025SaveLearn
Consistent truncation and generalized duality based on exceptional generalized cosetsWe present a systematic framework for constructing consistent truncations of supergravity based on exceptional generalized cosets of the form G/H. This approach generalizes the…Falk Hassler, Yuho Sakatani·Oct 14, 2025SaveLearn
Marginally deformed AdS5/CFT4 and spindle-like orbifoldsIn this thesis, the AdS/CFT correspondence is used as a tool to explore novel AdS5 Supergravity backgrounds (containing five-dimensional Anti-de Sitter spacetime) and their dual (four dimensional)…Paul Merrikin·Oct 14, 2025SaveLearn
de Sitter versus Anti de Sitter flows and the (super)gravity landscape: Part IIGeneric solutions are studied in Einstein-scalar gravity in an ansatz that can interpolate between de Sitter and Anti-de Sitter regimes. The scalar potential is arbitrary. All solutions are…Elias Kiritsis, Sergio Morales-Tejera, Christopher Rosen·Oct 14, 2025SaveLearn
The probe limit in MHD and its implications for magnetic transportMany phenomenological and effective field-theoretical (EFT) applications of magnetohydrodynamics (MHD) in the presence of a background magnetic field employ a simplifying assumption whereby the…Giorgio Frangi, Matej Bajec, Guri K. Buza et al.·Oct 14, 2025SaveLearn
Causal Bounds on EFTs with anomalies with a Pseudoscalar, Photons, and GravitonsTheories with pseudoscalars that couple through anomalies (such as axion models) are of particular phenomenological interest. We carry out a comprehensive analysis of all bounds obtainable from…Ziyu Dong, Jaehoon Jeong, Alex Pomarol·Oct 14, 2025SaveLearn
Nonconformally Ricci-flat instantons in Conformal Gravity with and without nonlinear matter fieldsIn this work, we study nonconformally Ricci-flat gravitational instantons in four-dimensional Conformal Gravity, both in vacuum and in the presence of nonlinear conformal matter. First, the…Cristóbal Corral, Borja Diez, Eleftherios Papantonopoulos·Oct 13, 2025SaveLearn
Sequestered Conformal Anomaly Mediation (SCAM)Supersymmetric models in singular extra dimensional spaces feature prominently in many interesting phenomenological models, including those derived from string theory. In this paper we explicitly…Michael Nee, Lisa Randall·Oct 13, 2025SaveLearn
Evolution With(out) Time: Relational Holography & BPS Complexity Growth in N=2 Double-Scaled SYKHow do we describe non-trivial bulk measurements relative to an observer (i.e. relationally) when both the observer and the system it probes may/may not evolve in time? How can we interpret this…Sergio E. Aguilar-Gutierrez·Oct 13, 2025SaveLearn
Scattering in the dual regime of Yang-Baxter deformed O(2N) sigma modelsWe continue to explore the previously suggested dual regime of Yang-Baxter (YB) deformed O(2N) sigma models, which is a new one-parametric deformation of the O(2N) model. It can…Alexey Bychkov, Boris Nekrasov·Oct 13, 2025SaveLearn