Stochastic thermodynamics for classical non-Markov jump processesStochastic thermodynamics investigates energetic and entropic bounds in small systems, but its foundational results rely on the Markov (memoryless) assumption. Although the Markov assumption is…Kiyoshi Kanazawa, Andreas Dechant·Aug 4, 2026SaveLearn
Two dimensional inhomogeneous classical systems at criticalityWe study simple inhomogeneous deformations of known two-dimensional classical lattice models described by conformal field theory (CFT) at large distances. The deformations are chosen to vary slowly…Jean-Marie Stéphan·Aug 3, 2026SaveLearn
Two-Parameter Ansatz for the Violation of Eigenstate ThermalizationThe eigenstate thermalization hypothesis (ETH) provides the prevailing framework for understanding quantum thermalization and ergodicity in isolated many-body systems. Yet, no general theory…Kohei Ohgane, Lev Vidmar·Aug 3, 2026SaveLearn
Fractal deconfinement and confinement in Sierpinski iceWe study the six-vertex model on the Sierpinski gasket, a four-coordinated hierarchical fractal with Hausdorff dimension df=23. Given the importance of dimensionality for the long-wavelength…James Walkling, Roderich Moessner·Aug 3, 2026SaveLearn
Universal crossovers in weakly-monitored quantum critical statesWe study post-measurement ensembles of ground states of tricritical and critical 1D quantum Ising Hamiltonians subjected, respectively, to weak energy and spin measurements without post-selection.…Abhishek Kumar, Rushikesh A. Patil, Andreas W. W. Ludwig et al.·Aug 3, 2026SaveLearn
Quantum resetting with memoryWe introduce a quantum stochastic resetting protocol with uniform memory, in which each resetting event returns the system to a state visited at a time chosen uniformly from its entire history. The…Gabriele de Mauro, Manas Kulkarni, Satya N. Majumdar·Aug 3, 2026SaveLearn
Renormalization-Group Stability Does Not Determine Front SelectionThe Fisher-Kolmogorov-Petrovsky-Piskunov (FKPP) equation provides a paradigmatic example of front propagation and asymptotic-state selection. Using a unified renormalization-group (RG) framework, we…Ko Okumura·Aug 3, 2026SaveLearn
Inhomogeneous Ising Model on 2D kagomé Lattice: Fermionic field approachWe investigate the two-dimensional inhomogeneous Ising model (2DIM) on the kagom'e lattice by mapping it onto a particular non-symmetric eight-vertex model and constructing the corresponding…Shahane A. Khachatryan, Zhidong Zhang, Ara G. Sedrakyan·Aug 3, 2026SaveLearn
Gap distributions between successive personal bests in cricket: Data and ModelsSuccessive personal best performances provide a natural measure of progression in an athlete's career. Classical record theory predicts a universal gap distribution, P(g) 1/g, for…Priyanka D. Bhoyar, Prashant M. Gade·Aug 3, 2026SaveLearn
Universal Scaling of the Magnetocaloric Effect in 2D Ising Monolayers and BilayerWe report a Monte Carlo study of the magnetocaloric effect (MCE) in two-dimensional ferromagnetic Ising models on square, honeycomb, and triangular lattices with monolayer and bilayer configurations.…Basit Iqbal, Kingshuk Sarkar·Aug 3, 2026SaveLearn
LieStoNet: Learning Lie Symmetries from Spatiotemporal Data for Stochastic Dynamical SystemsSymmetry is central to modern machine learning and physics: invariances and equivariances improve sample efficiency, robustness, and out-of-distribution generalization, while symmetry principles…Shida Liu, Abhishek Gupta, Sumit Sinha et al.·Aug 3, 2026SaveLearn
Spindrift: Learning quantum degeneracy from thermal purity in restricted path integral Monte CarloRestricted path integral Monte Carlo (RPIMC) sidesteps the fluctuating Fermion sign problem by confining paths within nodal regions of a trial density matrix, thereby recovering polynomial scaling.…Jarvist Moore Frost·Aug 3, 2026SaveLearn
Quantum Density of States and Integer Partitions: A Semiclassical ApproachIn this review we discuss semi-classical methods that are traditionally used to describe many-body systems in physics, but may also be used to describe partitions of integers in analytic number…M. V. N. Murthy, Matthias Brack·Aug 3, 2026SaveLearn
A universal emulator for planar Ising latticesWe introduce the notion of an Ising emulator for two-dimensional Ising models: flat, unit-edge-length lattices can be represented as site- or bond-diluted supercells of a single host lattice, for…Riccardo Ben Alì Zinati, Alessandro Codello·Aug 3, 2026SaveLearn
Streaming Molecular Dynamics Simulation Data for On-the-fly Processing and AnalysisOnly a small fraction of the data generated in state-of-the-art all-atom multi-microsecond molecular dynamics (MD) simulations is typically analyzed. With femtosecond integration steps, microsecond…Amruthesh Thirumalaiswamy, Lawson J. Woods, Heekun Cho et al.·Aug 3, 2026SaveLearn
A probabilistic framework for irreversible kineticsA probabilistic framework for irreversible kinetics is proposed in which a constrained path functional J encodes constitutive physics and observations on the admissible history space…Manas V. Upadhyay·Aug 3, 2026SaveLearn
Phase-space networks and connectivity of the kagome antiferromagnetWe study the coplanar ground-state manifold of the kagome Heisenberg antiferromagnet using a phase-space network representation, in which nodes correspond to coplanar ground states and edges…Brandon B. Le, Seung-Hun Lee, Gia-Wei Chern·Aug 3, 2026SaveLearn
Non-Markovian escape under stochastic resettingStochastic resetting is a powerful strategy known to optimize target-search processes at microscopic scales. While its effects on Markovian systems are well understood, its influence on memory-driven…Debasish Saha, Rati Sharma·Aug 3, 2026SaveLearn
Algorithmic overlaps in the Baxter-Wu model: cluster dynamics under Novotny-Evertz updatesWe study the spatial overlap of successive spin configurations generated by Markov chain Monte Carlo simulations of the Baxter-Wu model. Using the Novotny-Evertz sublattice-freezing single-cluster…Ian Pilé, Lev Shchur·Aug 2, 2026SaveLearn
Noise-enhanced temporal boundary states in non-Hermitian systemsTime-periodic modulation introduces a synthetic degree of freedom to manipulate topological phases. This synthetic dimension can trigger a phase transition that localizes a boundary state at the…Jielong Zhang, Bozheng Xue, Xianfeng Man et al.·Aug 2, 2026SaveLearn
Ultrametric organization of energy landscapes on random Erdős--Rényi graphs: topological origin of barrier hierarchyIn the present work, we investigate the hypothesis of the ultrametric organization of abstract energy landscapes defined on random Erdős--Rényi graphs. Within the proposed model, each vertex of the…A. P. Zubarev·Aug 2, 2026SaveLearn
Universality Emerging in a Universality: Derivation of the Ericson Transition in Stochastic Quantum Scattering and Experimental ValidationAt lower energies, the resonances in scattering experiments are often isolated. In quantum chaotic many-body, disordered or generically stochastic systems, the resonances overlap at larger energies.…Simon Köhnes, Jiongning Che, Barbara Dietz et al.·Aug 2, 2026SaveLearn
Non-perturbative constraints on stability and renormalization group flows in nonequilibrium matterWe derive constraints on renormalization group (RG) flows and stability of phases in nonequilibrium systems using quantum information inequalities. These constraints involve conditional mutual…Yu-Hsueh Chen, Tarun Grover·Aug 2, 2026SaveLearn
Scaling features in the Olami-Feder-Christensen modelWe consider the Olami-Feder-Christensen (OFC) model on a square lattice with open boundary conditions. The model exhibits self-organized criticality and explains the Gutenberg-Richter law observed…Naveen Kumar, Rahul Chhimpa, Avinash Chand Yadav·Aug 1, 2026SaveLearn
Memory with Onsager-Casimir symmetry: Rotating particle in a viscoelastic fluidWe study the stochastic dynamics of a rotating Brownian particle in a non-Markovian fluid. Experimentally, we find that rotation enhances the long-time diffusivity of the particle and generates…Debankur Das, Niloyendu Roy, Niklas Windbacher et al.·Jul 31, 2026SaveLearn