Dirac string

E569023

A Dirac string is a theoretical, unobservable line-like singularity in the electromagnetic potential that allows a magnetic monopole to exist consistently in quantum theory.

All labels observed (1)

Label Occurrences
Dirac string canonical 2

How this entity was disambiguated

Statements (45)

Predicate Object
instanceOf gauge artifact ⓘ
line singularity ⓘ
theoretical construct in quantum field theory ⓘ
topological defect (idealized) ⓘ
appearsInEquation A_φ potential of Dirac monopole in spherical coordinates ⓘ
appearsInTheory Dirac monopole theory ⓘ
U(1) gauge theory with magnetic charge ⓘ
quantum electrodynamics ⓘ
category concept in gauge theory ⓘ
concept in mathematical physics ⓘ
concept in theoretical physics ⓘ
conditionForUnobservability Dirac quantization condition e g = 2π n (in natural units) ⓘ
describedAs semi-infinite line attached to a magnetic monopole ⓘ
string of singular gauge potential extending from monopole ⓘ
existsOnlyIn potential description, not in field strength ⓘ
fieldStrengthProperty electromagnetic field tensor is regular away from monopole ⓘ
gaugeChoiceProperty can be hidden by using multiple gauge patches ⓘ
location can be moved by gauge transformation ⓘ
hasProperty carries no observable magnetic field except at monopole ⓘ
gauge-dependent ⓘ
line-like singularity in vector potential ⓘ
mathematical artifact required for monopole description ⓘ
unobservable in physical measurements ⓘ
introducedBy Paul Dirac ⓘ
introducedInContext quantization of magnetic charge ⓘ
introducedInYear 1931 (Dirac monopole paper) ⓘ
mathematicalRole allows definition of monopole magnetic field from a vector potential ⓘ
represents singular gauge transformation line ⓘ
namedAfter Paul Dirac ⓘ
observabilityCondition phase change around string must be integer multiple of 2π ⓘ
physicalInterpretation no direct observable consequences if charge quantization holds ⓘ
unphysical artifact removable by gauge choice ⓘ
quantumMechanicalRole affects phase of charged particle wavefunction around string ⓘ
relatedToConcept Aharonov–Bohm phase (formal analogy) ⓘ
Dirac quantization condition ⓘ
Wu–Yang monopole ⓘ
linked to: Yang monopole

fiber bundle description of monopoles ⓘ
gauge potential ⓘ
magnetic monopole ⓘ
vector potential singularity ⓘ
singularityLocationExample θ = 0 (positive z-axis) in alternative gauge ⓘ
θ = π (negative z-axis) in standard Dirac monopole gauge ⓘ
topologicalRole represents nontrivial first Chern class of U(1) bundle ⓘ
usedFor constructing monopole vector potentials ⓘ
deriving charge quantization from single-valued wavefunctions ⓘ

How these facts were elicited

Referenced by (2)

Full triples — surface form annotated when it differs from this entity's canonical label.