Stationary States for Fermions in an External Electric Field

Fuente: arXiv
Saved in:
Bibliographic Details
Main Authors: Zhao, Xuan, Wang, Yi, Zhuang, Pengfei
Format: Preprint
Published: 2025
Subjects:
Online Access:
Tags: Add Tag
No Tags, Be the first to tag this record!
_version_ 1866917465623101440
author Zhao, Xuan
Wang, Yi
Zhuang, Pengfei
author_facet Zhao, Xuan
Wang, Yi
Zhuang, Pengfei
contents We present a relativistic analysis of fermions in an external electric field by non-perturbatively solving the Dirac equation with a static gauge. Different from the magnetic field effect, the fermion wave function in an electric field oscillates asymptotically, which results in the absence of bound states in an infinite system. For a confined fermion, the confinement is gradually canceled by the electric field, and the fermion becomes deconfined when the electric coupling is stronger than the confinement coupling. However, a fermion in an electric field can be confined to a finite system by applying the MIT bag boundary condition, namely, the disappearing normal component of the probability current at the boundary. The solutions obtained can serve as a basis for calculating dynamical processes in the presence of a strong electric field, such as those occurring in the early stage of relativistic heavy-ion collisions, where an extremely strong electric field is expected to be generated.
format Preprint
id arxiv_https___arxiv_org_abs_2508_17757
institution arXiv
publishDate 2025
record_format arxiv
spellingShingle Stationary States for Fermions in an External Electric Field
Zhao, Xuan
Wang, Yi
Zhuang, Pengfei
Nuclear Theory
We present a relativistic analysis of fermions in an external electric field by non-perturbatively solving the Dirac equation with a static gauge. Different from the magnetic field effect, the fermion wave function in an electric field oscillates asymptotically, which results in the absence of bound states in an infinite system. For a confined fermion, the confinement is gradually canceled by the electric field, and the fermion becomes deconfined when the electric coupling is stronger than the confinement coupling. However, a fermion in an electric field can be confined to a finite system by applying the MIT bag boundary condition, namely, the disappearing normal component of the probability current at the boundary. The solutions obtained can serve as a basis for calculating dynamical processes in the presence of a strong electric field, such as those occurring in the early stage of relativistic heavy-ion collisions, where an extremely strong electric field is expected to be generated.
title Stationary States for Fermions in an External Electric Field
topic Nuclear Theory
url https://arxiv.org/abs/2508.17757