630 papers
Hep-Lat, short for High Energy Physics – Lattice, explores the fundamental forces of nature by simulating particle interactions on a digital grid. Instead of relying solely on abstract equations, researchers in this field use powerful computers to model how quarks and gluons bind together, offering deep insights into the structure of matter that are often impossible to derive analytically.
Gist.Science ensures these complex discoveries from arXiv remain accessible to everyone. We process every new preprint in this category as it is posted, providing both plain-language explanations for the curious and detailed technical summaries for experts. This dual approach bridges the gap between cutting-edge simulation work and broader scientific understanding.
Below are the latest papers in High Energy Physics – Lattice, curated directly from arXiv and ready for you to explore.
This paper presents a brief biography of William A. Bardeen (1941–2025), an American theoretical physicist at Fermilab renowned for his foundational contributions to the chiral anomaly, quantum chromodynamics, dynamical electroweak symmetry breaking, and heavy-light quark bound states.
This paper introduces a multiscale generative sampler that combines conditional Gaussian mixture models and masked continuous normalizing flows to overcome critical slowing down in lattice field theories, achieving significantly reduced autocorrelation times and enabling unbiased Multilevel Monte Carlo variance reduction for the two-dimensional scalar theory near criticality.
This paper compares the pion decay width in a uniform magnetic field calculated via chiral perturbation theory with lattice QCD results, finding consistency at large magnetic fields while attributing discrepancies at weak fields to differences in pion decay constants.
This paper utilizes QCD sum rule methods to model the resonance as a all-charm tetraquark in a diquark-antidiquark configuration, calculating its mass and decay widths to demonstrate consistency with experimental data and support its interpretation as a tensor state.
This paper presents an extended lattice study of SU(2) gauge theories with one and two adjoint fermion flavors, utilizing multiple methods to demonstrate that both theories reside in the conformal window with chiral symmetry unbroken, yielding continuum-limit anomalous dimensions of approximately 0.170 and 0.291, respectively.
This paper presents a lattice gauge theory formulation that successfully captures the continuum Atiyah-Patodi-Singer index for Dirac operators on domains with compact boundaries by exploiting its equivalence to the spectral flow of generalized domain-wall fermion operators, proving its validity for sufficiently small lattice spacings.
This paper critiques Henry Lamm's manuscript "Ether of Orbifolds" for incorrectly interpreting the quantity as a measure of gauge violation or departure from SU(), clarifying instead that it characterizes the shift in effective lattice spacing and that the associated claims about simulation costs are unfounded.
This paper investigates how fluctuating domain walls in the three-dimensional Ising model modify bulk observables through an effective interaction with the lightest massive mode, identifying a controlled regime governed by a renormalized coupling and validating these universal predictions via Monte Carlo simulations.
This paper demonstrates that lattice Maxwell theory with a -term in a modified Villain formulation exhibits an exact SL(2,Z) duality by employing a non-local transformation within the S-transformation to eliminate non-locality in the absence of monopoles, resulting in a structure for Wilson loops that closely resembles that of non-spin Maxwell theory.
Using modified Villain discretization on both Euclidean lattices and quantum chains, this paper demonstrates that non-invertible topological interfaces arising from flat gauging and T-duality in the two-dimensional compact boson survive discretization by generating non-compact edge modes with infinite quantum dimension, while also showing how these modes can be compactified at rational radii to yield standard defects with finite quantum dimension.