1985
DOI: 10.1007/bf00670815
|View full text |Cite
|
Sign up to set email alerts
|

Wave equation for a magnetic monopole

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

2
46
1
1

Year Published

1987
1987
2016
2016

Publication Types

Select...
5
2

Relationship

0
7

Authors

Journals

citations
Cited by 52 publications
(50 citation statements)
references
References 21 publications
2
46
1
1
Order By: Relevance
“…A physical interpretation of the associated effective functional energy equation (21) of [6] can be achieved by considering the classical limit of this equation. In this classical limit the system is described by its classical equations of motion.…”
Section: Effective Canonical Equations Of Motionmentioning
confidence: 99%
See 2 more Smart Citations
“…A physical interpretation of the associated effective functional energy equation (21) of [6] can be achieved by considering the classical limit of this equation. In this classical limit the system is described by its classical equations of motion.…”
Section: Effective Canonical Equations Of Motionmentioning
confidence: 99%
“…In this classical limit the system is described by its classical equations of motion. These equations of motion can be exactly derived from equation (21) of [6], if correlations in the matrix elements are suppressed. For details of the corresponding deduction we refer to [13], section 7.5 for instance.…”
Section: Effective Canonical Equations Of Motionmentioning
confidence: 99%
See 1 more Smart Citation
“…We remark that (5.21) has been called the Hertz theorem in [32,37] and it has been used there and also in [8,9,10,16,20,31,33] in order to find nontrivial superluminal solutions of the free Maxwell equation.…”
Section: Hertz Theorem the Hertz Potential Satisfiesmentioning
confidence: 99%
“…Under this condition, (6.27) becomes These results show that when a Dirac-Hestenes spinor field associated with the first of the Seiberg-Witten equations is in an eigenstate of the parity operator, that spinor field describes a pair of particles with opposite charges. We interpret these particles (following Lochak [16] who suggested that an equation equivalent to (8.10) describes massless monopoles of opposite charges) as being massless monopoles in auto-interaction. Observe that our proposed interaction is also consistent with the third of Seiberg-Witten equations, for F = dA implying a null magnetic current.…”
Section: Derivation Of Seiberg-witten Equationsmentioning
confidence: 99%