Titlebook: Classical Field Theory; On Electrodynamics, Florian Scheck Textbook 20121st edition Springer-Verlag Berlin Heidelberg 2012 General Relativ

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Andrey V. Mehrentsev,Artem V. Kruglov and the principle of universal conservation of electric charge. These laws can be tested – confirmed or falsified – in realistic experiments. The integral form of the laws deals with physical objects that are one-dimensional, two-dimensional, or three-dimensional, that is to say, objects such as li

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Andrey V. Mehrentsev,Artem V. Kruglov Maxwell’s equations show interesting transformation properties under continuous and discrete spacetime transformations. However, only the action of the whole Lorentz group on them reveals their full symmetry structure. A good example that illustrates the covariance of Maxwell’s equations is provide

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Zehua Fu,Mohsen Ardabilian,Guillaume Sternith a finite number of degrees of freedom. Hamilton’s principle characterizes the physically realizable orbits, among the set of all possible orbits, as being the critical elements of the action integral. The Lagrangian function, although not an observable on its own, is not only useful in deriving

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Andrey V. Mehrentsev,Artem V. Kruglovs equations. These case studies are restricted to the classical, nonquantized version of the theory. The field of semiclassical interactions of quantum matter and classical radiation field, as well as the full quantum field-theoretic treatment of Maxwell theory is described in many monographs or tex

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Hela Haj Mohamed,Samir Belaid,Wady Naanaaerpretation only in relation to quantum mechanics of electrons and the Schrödinger equation. In this chapter, we study the generalization of the concept of a locally invariant gauge theory to non-Abelian gauge groups constructed by following the model of Maxwell theory. This generalization may seem

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Hela Haj Mohamed,Samir Belaid,Wady Naanaaold which is a Euclidean space and which locally is decomposable into a direct product .. = ℝR. ℝR of a physical space ℝR.. of motions, and a time axis ℝR.. The first factor is the threedimensional space as it is perceived by an observer at rest while the time axis displays the (coordinate) time tha

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https://doi.org/10.1007/978-3-642-27985-0General Relativity; Maxwell Theory; Riemann Geometry; non-Abelian gauge theories; rnetamaterials with ne

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978-3-642-43128-9Springer-Verlag Berlin Heidelberg 2012

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Classical Field Theory978-3-642-27985-0Series ISSN 1868-4513 Series E-ISSN 1868-4521

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Andrey V. Mehrentsev,Artem V. Kruglovs equations. These case studies are restricted to the classical, nonquantized version of the theory. The field of semiclassical interactions of quantum matter and classical radiation field, as well as the full quantum field-theoretic treatment of Maxwell theory is described in many monographs or textbooks, such as, for example, [QP].