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Lattice quantum electrodynamics in (3+1)-dimensions at finite density with tensor networks
Giuseppe Magnifico1,2, Timo Felser3,4,5, Pietro Silvi6,7
1Dipartimento di Fisica e Astronomia G. Galilei, Università di Padova, Padova, Italy. giuseppe.magnifico@unipd.it.
Tensor Network simulations overcome the sign-problem in gauge theories, enabling the study of quantum electrodynamics at finite charge densities. This research characterizes collective phases and confinement effects without numerical limitations.
Area of Science:
- * Fundamental particle physics and quantum field theory.
- * Computational physics and condensed matter theory.
Background:
- * Gauge theories are crucial for understanding matter and interactions.
- * Non-perturbative effects and phase diagrams, especially at finite charge density, remain challenging due to the sign-problem in numerical simulations.
Purpose of the Study:
- * To apply Tensor Network methods for sign-problem-free simulations of lattice gauge theories.
- * To investigate the ground states and phase diagram of compact Quantum Electrodynamics (QED) with dynamical matter.
- * To explore collective phases, confinement, and charge-screening effects at zero and finite charge densities.
Main Methods:
- * Employed Tensor Network simulations in the Hamiltonian formulation.
- * Simulated a three-dimensional lattice gauge theory including dynamical matter.
- * Addressed sign-problem limitations inherent in traditional Monte Carlo methods.
Main Results:
- * Successfully simulated ground states of compact QED using a sign-problem-free approach.
- * Characterized collective phases of the model at varying charge densities.
- * Investigated the presence of a confining phase at large gauge coupling and analyzed charge-screening effects.
Conclusions:
- * Tensor Network simulations provide a viable, sign-problem-free alternative for studying gauge theories with dynamical matter.
- * The study offers new insights into the phase structure and properties of compact QED, particularly at finite densities.
- * This methodology opens avenues for exploring complex non-perturbative phenomena in quantum field theory.
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