Dissipation-coherence tradeoff for stochastic oscillationsAutonomous noisy oscillations in biochemical and mesoscopic systems require nonequilibrium driving and therefore dissipation. A striking conjecture by Oberreiter, Barato, and Seifert (OBS) proposes a…Jie Gu·Jun 3, 2026SaveLearn
Opinion dynamics on social proximity disordered networksUnderstanding how local social pressure shapes collective opinion formation is essential in modern society, with implications in sociology, politics, finance, and technology. Complex networks are a…Fellipe Aranha, Giuliano G. Porciúncula, Adauto J. F. de Souza et al.·Jun 3, 2026SaveLearn
Adiabatic Ramp Dynamics Across the ETH--MBL Transition in Disordered XXZ Spin ChainMany-body localization(MBL) provides a mechanism by which isolated interacting quantum systems with disorder can avoid thermalization unlike ergodic systems satisfying the eigenstate thermalization…Nidhi Kumari, Vinod Ashokan·Jun 3, 2026SaveLearn
Proof of entropic order in Generalized Ising ModelsOrdering at arbitrarily high temperature - entropic order - has been argued to take place in a class of generalized Ising models parameterised by a real interaction parameter p when p 1. We…Enrico Andriolo, Mendel Nguyen, Emily Richards et al.·Jun 3, 2026SaveLearn
Spectral Duality and Thermodynamic Bounds on Finite-frequency Fluctuation ResponsesFluctuation-response relations encode fundamental constraints on non-equilibrium systems. While time-domain static response is bounded by activity and entropy production, finite-frequency…Jiming Zheng, Zhiyue Lu·Jun 3, 2026SaveLearn
Spontaneous Symmetry Breaking in Two-dimensional Long-range Heisenberg ModelAlgebraically decaying interactions 1/rd+σ can lead to nontrivial universality beyond short-range (SR) theories and spontaneous symmetry breaking in low-dimensional systems. We perform…Tianning Xiao, Dingyun Yao, Lode Polle et al.·Jun 3, 2026SaveLearn
Monotonicity of eigenstate thermalization hypothesis in two-dimensional systemsWe study numerically the enveloping f-function of the fluctuation term in eigenstate thermalization hypothesis (ETH) statement. We concentrate on the energy (or entropy) dependence of this function…Nilakash Sorokhaibam, Anjan Daimari·Jun 3, 2026SaveLearn
Constraint-Enhanced Physical Search through Correlation MatchingPhysical systems do not merely add noise to search processes; they impose constraints that generate structured correlations. We propose a principle of constraint-enhanced physical search in which…Song-Ju Kim·Jun 2, 2026SaveLearn
A proof of an identity for the critical exponents of jammingWithin the full replica-symmetry-breaking (fullRSB) solution of dense hard spheres in infinite dimension, Charbonneau, Kurchan, Parisi, Urbani, and Zamponi (CKPUZ; J.Stat.Mech.P10009, 2014)…Giorgio Parisi, Francesco Zamponi·Jun 2, 2026SaveLearn
Kinetic energy in random recurrent neural networksHigh-dimensional chaotic dynamics can emerge in a large random recurrent neural network when the synaptic gain crosses a threshold. Recent works showed that the kinetic energy of neural activity…Li-Ru Zhang, Haiping Huang·Jun 2, 2026SaveLearn
Fractionally Quantized Recurrence Detection Times in Monitored Quantum Many-Body SystemsRecurrence time quantifies the duration required for a physical system to return to its initial state, playing a pivotal role in understanding the predictability of complex systems. In quantum…Quancheng Liu, Sabine Tornow, David A. Kessler et al.·Jun 2, 2026SaveLearn
Electromagnetic Field Equivalence from Moving ManifoldsWe apply a geometric formulation of electromagnetic fields on moving manifolds to the problem of field equivalence between dynamically separated domains. Starting from the tensorially invariant…David V. Svintradze·Jun 1, 2026SaveLearn
Linear optimal protocol for physical constraints in weakly driven processesThe minimization of irreversible work in weakly driven systems within linear response under physical constraints on the protocol derivative is studied. The problem reduces to a shifted eigenvalue…Pierre Nazé·Jun 1, 2026SaveLearn
Can the Brownian diffusion coefficient be reconstructed from Lyapunov exponents?We consider an ac-driven particle moving in a spatially periodic and symmetric potential. In the zero- temperature limit, for the analyzed parameter set, its dynamics is non-chaotic and the particle…I. G. Marchenko, I. I. Marchenko, D. Ivashchenko et al.·Jun 1, 2026SaveLearn
Role of System-Bath Interaction in Non-Markovian Quantum Brownian Otto CyclesWe study finite-time quantum Otto cycles whose working medium is a harmonic oscillator undergoing a quantum Brownian motion described by the Caldeira-Leggett model when the oscillator is in contact…Haena Shim, Joonhyun Yeo·Jun 1, 2026SaveLearn
Tandem Exclusion ProcessWe introduce the tandem exclusion process (TEP), a one-dimensional stochastic lattice model motivated by tandem running in ants. Particles evolve through two cooperative local transitions,…Ngo Phuoc Nguyen Ngoc, Lam Thi Nhung, Huynh Anh Thi·Jun 1, 2026SaveLearn
Physical completion of the Navier-Stokes equationsThe incompressible Navier-Stokes equations contain viscous dissipation but no thermal noise. I show, using a topological argument based on Poincaré's lemma, that the fluctuation-dissipation…Samuel L. Braunstein·Jun 1, 2026SaveLearn
Hyperuniformity in active fluids reshapes nucleation and capillary-wave dynamicsWhile nucleation in typical active and driven fluids often appears equilibrium-like, striking departures emerge when large-scale fluctuations are strongly suppressed. Here, we investigate nucleation…Raphaël Maire·Jun 1, 2026SaveLearn
Optimal active engines obey the thermodynamic Lorentz force lawWhat are the fundamental limitations for finite-time engines that extract work from active nonequilibrium systems, and what are the optimal protocols that approach them? We show that the finite-time…Adrianne Zhong, Adam G. Frim, Michael R. DeWeese·Jun 1, 2026SaveLearn
Typicality of thermal states in isolated quantum systems corresponds to ubiquity of global minima in wide artificial neural networksThe Neural Tangent Kernel theory theoretically guarantees the existence of global minima of the cost functional in the neighborhood of an arbitrary random initialized parameters in wide artificial…Takaaki Monnai·Jun 1, 2026SaveLearn
Weak-Memory Dynamics in Discrete TimeDiscrete dynamics arise naturally in systems with broken temporal translation symmetry and are typically described by first-order recurrence relations representing classical or quantum Markov chains.…Hugues Meyer, Kay Brandner·Jun 1, 2026SaveLearn
Minimal-Dissipation Learning for Energy-Based ModelsWe show that the bias of the approximate maximum-likelihood estimation (MLE) objective of a persistent chain energy-based model (EBM) is precisely equal to the thermodynamic excess work of an…Jeff Hnybida, Simon Verret·Jun 1, 2026SaveLearn
Pushing-Induced Arrest Across Lattices and DimensionsTracer-media interactions can give rise to transport phenomena beyond classical models; e.g., obstacle pushing can eliminate percolation. We demonstrate that the existing "snowplow" mechanism…Itamar Shitrit, Ofek Lauber Bonomo, Shlomi Reuveni·May 31, 2026SaveLearn
Nonlinearity-induced transition in heat conduction through a topological metamaterial of rotorsWe investigate heat conduction in a one-dimensional chain of rigid rotors. The rotors are constrained to rotate in a plane about fixed pivot points and coupled by springs, such that in equilibrium,…T. R. Vishnu, Dibyendu Roy·May 31, 2026SaveLearn
Long-Range Order in a Strictly Short-Range Quasi-2D XY Model: When Critical Fluctuations MatterThe phase of spins in the quasi-two-dimensional (q2D) XY model has emerged as a topic of significant interest across multiple subfields of physics. Conventional wisdom, rooted in the Mermin-Wagner…Minghui Hu, Chao Zhang, Dajun Zhang et al.·May 31, 2026SaveLearn