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Reconstruction of Macroscopic Maxwell Equations [electronic resource] : A Single Susceptibility Theory / by Kikuo Cho.

By: Contributor(s): Series: Springer Tracts in Modern Physics ; 237Publisher: Berlin, Heidelberg : Springer Berlin Heidelberg : Imprint: Springer, 2010Description: XIV, 138 p. 7 illus. online resourceContent type:
  • text
Media type:
  • computer
Carrier type:
  • online resource
ISBN:
  • 9783642127915
Subject(s): Genre/Form: Additional physical formats: Printed edition:: No titleDDC classification:
  • 530.15 23
LOC classification:
  • QC5.53
Online resources:
Contents:
New Form of Macroscopic Maxwell Equations -- Discussions of the New Results -- Further Considerations -- Mathematical Details and Additional Physics.
In: Springer eBooksSummary: This book presents a logically more complete form of macroscopic Maxwell equations than the conventional ones by applying long wavelength approximation to microscopic nonlocal theory. This scheme requires only one susceptibility tensor describing electric and magnetic polarizations together with their mutual interference. The quantum mechanical expression of the susceptibility covers both chiral and achiral symmetry. Only in the absence of chiral symmetry, this reduces to the conventional form, under the additional condition of using magnetic susceptibility defined with respect to, not H, but B. This scheme solves various problems inherent to the conventional scheme of Maxwell equations.
Item type: eBooks
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New Form of Macroscopic Maxwell Equations -- Discussions of the New Results -- Further Considerations -- Mathematical Details and Additional Physics.

This book presents a logically more complete form of macroscopic Maxwell equations than the conventional ones by applying long wavelength approximation to microscopic nonlocal theory. This scheme requires only one susceptibility tensor describing electric and magnetic polarizations together with their mutual interference. The quantum mechanical expression of the susceptibility covers both chiral and achiral symmetry. Only in the absence of chiral symmetry, this reduces to the conventional form, under the additional condition of using magnetic susceptibility defined with respect to, not H, but B. This scheme solves various problems inherent to the conventional scheme of Maxwell equations.

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