Quantum Field Theory of Particles with Both Electric and Magnetic Charges
Abstract
The quantum field theory of particles with both electric and magnetic charges is developed as an obvious extension of Schwinger's quantum field theory of particles with either electric or magnetic charge. Two new results immediately follow. The first is the chiral equivalence theorem which states the unitary equivalence of the Hamiltonians describing the system of particles with electric and magnetic charges ${e}_{n}$, ${g}_{n}$ and the system with charges ${{e}_{n}}^{\ensuremath{'}}=cos\ensuremath{\theta}$, ${e}_{n}+sin\ensuremath{\theta}{g}_{n}$, ${{g}_{n}}^{\ensuremath{'}}=\ensuremath{-}sin\ensuremath{\theta}{e}_{n}+cos\ensuremath{\theta}{g}_{n}$. This result holds in particular in the absence of physical magnetic charges. The second result is that if physical magnetic charges do occur, then, in consequence of chiral equivalence, the charge quantization condition applies, not to the separate products ${e}_{m}{g}_{n}$, but to the combinations ${e}_{m}{g}_{n}\ensuremath{-}{g}_{m}{e}_{n}$, which must be integral multiples of $4\ensuremath{\pi}$. The general solution of this condition leads to the introduction of a second elementary quantum of electric charge ${e}_{2}$, the electric charge on the Dirac monopole, besides the first elementary charge ${e}_{1}$, the charge on the electron. There are no other free parameters.
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Physically meaningful properties of the field should respect the Heaviside-Larmor symmetry.
“It follows that physically meaningful properties of the fi eld should also respect this symmetry [37] and this idea has been useful in deriving forms for the spin and orbital angular momenta of the fi eld [38, 39] and for its helicity [40 -45].”
From Optical Dirac equation (2014) · cites this paper as [42]
The required form of the helicity density within the optical Dirac equation is obtained by defining the helicity operator to be Σ·p/p^2, yielding the familiar expression.
“which is the familiar expression [40 -45, 78].”
From Optical Dirac equation (2014) · cites this paper as [42]
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- Authors
- Zwanziger, D.
- Affiliations
- New York University (US)
- Corresponding author
- Zwanziger, Daniel
- Venue
- Physical Review
- Publisher
- American Physical Society (APS)
- Published
- 1968-12-25
- Volume
- 176
- Issue
- 5
- Pages
- 1489-1495
- ISSN
- 0031-899X (ISSN-L)
- OpenAlex
- W2798042909
- Semantic Scholar
- 90831186b484ee6e27d36dd0c82fe75f042ebd19
- Cited by
- 343
- References
- 15
- Citations by year
- 2026: 5 · 2025: 7 · 2024: 9 · 2023: 46 · 2022: 12 · 2021: 12 · 2020: 7 · 2019: 11 · 2018: 11 · 2017: 5 · 2016: 8 · 2015: 10 · 2014: 10 · 2013: 13 · 2012: 12
- FWCI
- 2.95
- Type
- journal article
- Language
- en
- Open access
- closed
- Locations
- Physical Review (publishedVersion)
- Topics
- Physical Sciences › Physics and Astronomy › Atomic and Molecular Physics, and Optics › Quantum and Classical Electrodynamics
- Physical Sciences › Physics and Astronomy › Nuclear and High Energy Physics › Particle physics theoretical and experimental studies
- Physical Sciences › Physics and Astronomy › Nuclear and High Energy Physics › Black Holes and Theoretical Physics
- Keywords
- magnetic monopoles, electric and magnetic charges, Dirac monopole, charge quantization, elementary charge, Dirac quantization
About these checks
Registry, retraction, Cites and statistics results are computed, not judged, with one exception: a printed reference that no index lists is read once by a model before it counts as a citation error. Claims are extracted by a model and kept only when their quote appears verbatim in the text; each cited source is then checked, with a model’s help, for whether it says what the claim relies on. Those verdicts can be wrong — read the claim’s quote and the cited source before relying on one.
Statistics and arithmetic are recomputed, not judged.
Confidence bands are shown only for fields calibrated on our annotated test set. None is calibrated yet, so no band is shown.
What counts as a claim ›How we measure confidence ›How we check this ›
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