Euclidean Correlation Functions in Quantum GravityWe calculate Euclidean correlation functions through next-to-leading order in the low energy effective theory of gravity. We focus on correlation functions of curvature and volume operators,…Jack Laiho, Kenny Ratliff·Oct 13, 2025SaveLearn
GraviGUT unification with revisited Pati-Salam modelWe propose a graviGUT unification scheme based on the simple orthogonal group SO(1,9 ,C) that resolves the chiral duplication of weak isospin in Pati--Salam models. In the…Stephon Alexander, Bruno Alexandre, Michael Fine et al.·Oct 13, 2025SaveLearn
Hidden zeros for higher-derivative YM and GR amplitudes at tree-levelWe extend the recently discovered phenomenon of hidden zeros to tree amplitudes for Yang-Mills (YM) and general relativity (GR) theories with higher-derivative interactions. This includes gluon…Kang Zhou·Oct 13, 2025SaveLearn
A family of three maximally symmetric boost-invariant flows in relativistic hydrodynamicsI discuss the constructions of boost-invariant dissipative conformal hydrodynamic flows by elaborating on the geometric procedure by Gubser and Yarom, which starts from a static, maximally symmetric…Sašo Grozdanov·Oct 12, 2025SaveLearn
Two decades of algorithmic Feynman integral reductionWe present a historiographical review of algorithms and computer codes developed for solving integration-by-parts relations for Feynman integrals. This procedure is one of the key steps in the…Alexander Smirnov, Vladimir Smirnov·Oct 12, 2025SaveLearn
AdS3 Freelance Holography, A Detailed AnalysisFreelance holography program is an extension of the gauge/gravity correspondence in which the boundary theory can reside on any timelike codimension-one surface in AdS space, and the boundary…M. M. Sheikh-Jabbari, V. Taghiloo·Oct 12, 2025SaveLearn
Integrability in Three-Dimensional Gravity: Eigenfunction-Forced KdV FlowsWe uncover a direct connection between three-dimensional gravity with chiral boundary conditions and a class of forced integrable systems. Starting from the Chern-Simons formulation, we derive…Hamed Adami, Anouchah Latifi·Oct 12, 2025SaveLearn
Metallic transports from Taub-NUT AdS black holesWe compute holographic DC conductivity associated with the Taub-NUT-AdS4 black holes following the probe D-brane approach. In particular, we examine the effects of frame dragging on charge…Mohd Aariyan Khan, Hemant Rathi, Dibakar Roychowdhury·Oct 12, 2025SaveLearn
Newtonian potential from scattering amplitudes in super-renormalizable gravityBased on the classical limit of relativistic scattering amplitudes, we compute the coupling between a general super-renormalizable gravity and massive scalar particles. This allows us to derive the…Haiyuan Feng, Rong-Jia Yang, Jinjun Zhang·Oct 11, 2025SaveLearn
On thermal holographic RG flowsHolographic Renormalization Group (RG) flows, described by Einstein gravity coupled to matter fields, have been thoroughly explored in the context of vacuum states. In this work, we shift the focus…Elena Cáceres, Hare Krishna·Oct 11, 2025SaveLearn
Analytic results in conformal field theorySince the 1980s, many exact results have been discovered in 2d CFT, from critical exponents to correlation functions to complete solutions of certain models. In d>2, there is a wealth of…Philine van Vliet, Emilio Trevisani, Ingo Runkel et al.·Oct 10, 2025SaveLearn
Exact BPS double-kinks in generalized ϕ4, ϕ6 and sine-Gordon modelsWe consider a (1+1)-dimensional theory with a single real scalar field ϕ whose kinematics is modified by a generalizing function f(ϕ). After briefly reviewing its…R. Casana, E. da Hora, F. C. Simas·Oct 10, 2025SaveLearn
Unveiling dynamical quantum error correcting codes via non-invertible symmetriesDynamical stabilizer codes (DSCs) have recently emerged as a powerful generalization of static stabilizer codes for quantum error correction, replacing a fixed stabilizer group with a sequence of…Rajath Radhakrishnan, Adar Sharon, Nathanan Tantivasadakarn·Oct 10, 2025SaveLearn
Locating the Ising CFT via the ground-state energy on the fuzzy sphereWe locate the phase-transition line for the Ising model on the fuzzy sphere from a finite-size scaling analysis of its ground-state energy. Our strategy is to write the latter as $EGS(Nm)/Nm =…Kay Joerg Wiese·Oct 10, 2025SaveLearn
Analytic action principle in N=2 AdS4 harmonic superspaceWe develop the analytic action principle in the N=2 AdS4 harmonic superspace and apply it for studying the component structure of the free q-hypermultiplet model.Timothy Gargett, Igor Samsonov·Oct 10, 2025SaveLearn
Yukawa interactions in Quantum GravityWe present the first complete next-to-leading-order analysis of a Yukawa system within the framework of asymptotically safe quantum gravity. Our results are obtained through a systematic resummation…Gustavo P. de Brito, Manuel Reichert, Marc Schiffer·Oct 10, 2025SaveLearn
Quantization of charged fields in the presence of intense electromagnetic fieldsThis thesis applies techniques from quantum field theory in curved spacetimes to study particle creation in external fields, focusing on the Schwinger effect (i.e., the production of…Álvaro Álvarez-Domínguez·Oct 10, 2025SaveLearn
Non-closed scalar charge in four-dimensional Einstein-scalar-Gauss-Bonnet black hole thermodynamicsWe develop a covariant differential-form framework to define scalar charges for stationary, asymptotically flat black holes in 4--dimensional Einstein-scalar-Gauss-Bonnet gravity with a general…Romina Ballesteros, Marcela Cárdenas, Eric Lescano·Oct 9, 2025SaveLearn
There and Back Again: Bulk-to-Defect via Ward IdentitiesIn conformal field theory, the presence of a defect may break the global symmetry, giving rise to defect operators such as the tilts. In this work, we derive integral identities that relate…Jake Belton, Ziwen Kong·Oct 9, 2025SaveLearn
Exploring the Spectral Edge in SYK ModelsPrevious work on Jackiw-Teitelboim (JT) gravity has shown that, at low temperatures, the annealed entropy becomes negative and departs from the quenched entropy. From the perspective of the…Bowen Ouyang, Pratik Rath·Oct 9, 2025SaveLearn
Broken Weyl Gravity: Dynamical Torsion and Generalized ProcaWe develop a symmetry-based construction of gravity from a phase in which Weyl invariance is spontaneously broken. Using the coset formalism, the dilaton acts as a Stuckelberg field for the gauged…Lucas Fernández Sarmiento, Irvin Martínez Rodríguez·Oct 9, 2025SaveLearn
Tripartite entanglement in the HaPPY code is not holographicHolographic states satisfy several entropic inequalities owing to the Ryu-Takayangi formula. A drawback of these inequalities is that they only use bipartite entanglement in their formulation. We…Sriram Akella·Oct 9, 2025SaveLearn
CPT breaking in noncommutative Magueijo-Smolin modelWe review an instance of noncommutative geometry based on a specific realization of the model of doubly special relativity proposed by Magueijo and Smolin (MS) on noncommutative spacetime. In…S. Mignemi·Oct 9, 2025SaveLearn
The Rise of Linear TrajectoriesIn this letter, we consider constraints on the low-energy spectrum of amplitudes with higher-spin exchange. Assuming unitarity, crossing symmetry, and super-convergent high energy behavior,…Yu-tin Huang, Sara Ricossa, Francesco Riva et al.·Oct 9, 2025SaveLearn
Spinning Mellin amplitudesWe propose a definition of Mellin amplitudes for conformal correlators involving arbitrary spinning operators in tensor representations of the Lorentz group. These representations cover all bosonic…Zhongjie Huang, Yichao Tang·Oct 8, 2025SaveLearn