Abstract
The Lagrangian formalism has to be seen as the point of departure for classical field theories. This approach is also providing the scaffold for (canonical) quantum field theories. Instead of using a local notation, our representation of the formalism will be based upon differential forms which are globally defined on a pseudo-Riemannian manifold of dimension n.
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Notes
- 1.
Mack (1981) interpreted this postulate physically as a result of a “Naheinformationsprinzip”, regarding it as a generalization of the principle of action-at-close-distances.
- 2.
More generally, one could imagine the existence of topological modified Lagrangians \({\buildrel \theta \over L} =-(\cos \theta \,F\wedge \,^* F+\sin \theta \,F\wedge F)/2\), where \(\theta \) is the’vacuum’ angle of duality rotations or higher order functionals of the two quadratic invariants.
- 3.
The displacement current \(\partial \mathfrak {D}/\partial t\), where \(\mathfrak {D}=\varepsilon \mathbf {E}\), was anticipated 1839 by James Mac Cullagh, cf. Darrigol (2010). It later on turned out to be a necessary ingredient for rendering electromagnetism relativistic-invariant.
- 4.
In four dimensions, B resembles the two-form potential for the gauge-invariant field strength or excitation \(H=dB\), the Kalb–Ramond axion three-form.
- 5.
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Mielke, E.W. (2017). Maxwell and Yang–Mills Theory. In: Geometrodynamics of Gauge Fields. Mathematical Physics Studies. Springer, Cham. https://doi.org/10.1007/978-3-319-29734-7_3
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