Faraday’s Form and Maxwell’s Equations in the Heisenberg Group
Identifieur interne : 000570 ( Main/Exploration ); précédent : 000569; suivant : 000571Faraday’s Form and Maxwell’s Equations in the Heisenberg Group
Auteurs : Bruno Franchi [Italie] ; Maria Carla Tesi [Italie]Source :
- Milan Journal of Mathematics [ 1424-9286 ] ; 2009-12-01.
Abstract
Abstract: In this note we present a geometric formulation of Maxwell’s equations in Carnot groups (connected simply connected nilpotent Lie groups with stratified Lie algebra) in the setting of the intrinsic complex of differential forms defined by M. Rumin. Restricting ourselves to the first Heisenberg group $${\mathbb{H}^{1}}$$ , we show that these equations are invariant under the action of suitably defined Lorentz transformations, and we prove the equivalence of these equations with differential equations “in coordinates”. Moreover, we analyze the notion of “vector potential”, and we show that it satisfies a new class of 4th order evolution differential equations.
Url:
DOI: 10.1007/s00032-009-0104-9
Affiliations:
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<front><div type="abstract" xml:lang="en">Abstract: In this note we present a geometric formulation of Maxwell’s equations in Carnot groups (connected simply connected nilpotent Lie groups with stratified Lie algebra) in the setting of the intrinsic complex of differential forms defined by M. Rumin. Restricting ourselves to the first Heisenberg group $${\mathbb{H}^{1}}$$ , we show that these equations are invariant under the action of suitably defined Lorentz transformations, and we prove the equivalence of these equations with differential equations “in coordinates”. Moreover, we analyze the notion of “vector potential”, and we show that it satisfies a new class of 4th order evolution differential equations.</div>
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