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Faraday’s Form and Maxwell’s Equations in the Heisenberg Group

Identifieur interne : 000570 ( Main/Exploration ); précédent : 000569; suivant : 000571

Faraday’s Form and Maxwell’s Equations in the Heisenberg Group

Auteurs : Bruno Franchi [Italie] ; Maria Carla Tesi [Italie]

Source :

RBID : ISTEX:93AF769F43CE0F0A902705BE0DE46227DB5EFF4A

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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