How to Choose a Gauge? The Case of Hamiltonian Electromagnetism.

We develop some ideas about gauge symmetry in the context of Maxwell's theory of electromagnetism in the Hamiltonian formalism. One great benefit of this formalism is that it pairs momentum and configurational degrees of freedom, so that a decomposition of one side into subsets can be translated int...

Full description

Bibliographic Details
Published in:Erkenntnis Vol. 89; no. 4; pp. 1581 - 1616
Main Authors: Gomes, Henrique, Butterfield, Jeremy
Format: Article
Published: Springer Nature Apr2024
Subjects:
Online Access:View this record in EBSCOhost
fields @attributes:
  recordID: 1
pdfLink:
plink: https://search.ebscohost.com/login.aspx?direct=true&db=hlh&AN=176583024&site=ehost-live
header:
  @attributes:
    shortDbName: hlh
    uiTerm: 176583024
    longDbName: Humanities International Complete
    uiTag: AN
  controlInfo:
    bkinfo:
    jinfo:
      jid:
        01650106
        5KZ
      jtl: Erkenntnis
      issn: 01650106
      maglogo: N
    pubinfo:
      dt: Apr2024
      vid: 89
      iid: 4
      pid: 237
      pub: Springer Nature
    artinfo:
      ui:
        176583024
        10.1007/s10670-022-00597-9
      ppf: 1581
      ppct: 35
      formats:
        fmt:
          – @attributes:
              type: T
          – @attributes:
              type: P
              size: 1.7MB
      tig:
        atl: How to Choose a Gauge? The Case of Hamiltonian Electromagnetism.
      aug:
        au:
          Gomes, Henrique
          Butterfield, Jeremy
        affil: https://ror.org/013meh722 Trinity College, University of Cambridge, Cambridge, UK
      su:
        Helmholtz, Hermann von, 1821-1894
        Electromagnetism
        Degrees of freedom
        Equations of motion
        Electric fields
        Gauge symmetries
      sug:
        subj:
          Helmholtz, Hermann von, 1821-1894
          Electromagnetism
          Degrees of freedom
          Equations of motion
          Electric fields
          Gauge symmetries
      ab: We develop some ideas about gauge symmetry in the context of Maxwell's theory of electromagnetism in the Hamiltonian formalism. One great benefit of this formalism is that it pairs momentum and configurational degrees of freedom, so that a decomposition of one side into subsets can be translated into a decomposition of the other. In the case of electromagnetism, this enables us to pair degrees of freedom of the electric field with degrees of freedom of the vector potential. Another benefit is that the formalism algorithmically identifies subsets of the equations of motion that represent time-dependent symmetries. For electromagnetism, these two benefits allow us to define gauge-fixing in parallel to special decompositions of the electric field. More specifically, we apply the Helmholtz decomposition theorem to split the electric field into its Coulombic and radiative parts, and show how this gives a special role to the Coulomb gauge (i.e. div (A) = 0 ). We relate this argument to Maudlin's (Entropy, 2018. https://doi.org/10.3390/e20060465) discussion, which advocated the Coulomb gauge.
      pubtype: Academic Journal
      doctype: Article
      src: R
    language: English
    refInfo:
    copyright:
      @attributes:
        flag: Y
      custom: Erkenntnis is a copyright of Springer, 2024. All Rights Reserved.
      item: Erkenntnis
      holder: Springer Nature
      dt:
        @attributes:
          year: 2024
    holdings:
      @attributes:
        islocal: N