Read e-book online Photonic Crystals: Physics and Practical Modeling PDF

By Igor A. Sukhoivanov

ISBN-10: 3642026451

ISBN-13: 9783642026454

ISBN-10: 364202646X

ISBN-13: 9783642026461

The nice curiosity in photonic crystals and their purposes some time past decade calls for an intensive education of scholars and pros who can virtually follow the data of physics of photonic crystals including abilities of self reliant calculation of simple features of photonic crystals and modelling of assorted photonic crystal parts for software in all-optical communique structures. This e-book combines easy backgrounds in fiber and built-in optics with specific research of mathematical versions for 1D, 2nd and 3D photonic crystals and microstructured fibers, in addition to with descriptions of actual algorithms and codes for sensible consciousness of the models.

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Additional resources for Photonic Crystals: Physics and Practical Modeling

Example text

1) D (r, t) = εr (r) ε0 E(r, t), where μ is the vacuum permeability, and εr and ε0 are the relative permittivity and electric constant. As long as we suppose the medium to be non-magnetic, its relative permeability is equal to 1. Thus, the selected form of the equations pair is written down for the medium which is susceptible to the electric field and unsusceptible to the magnetic field. Writing the equations in the abovementioned form, we completely determined the variations of environment parameters.

1i*k*layerRI(length(layerRI))*... exp(1i*k*layerRI(length(layerRI))*xCurrent)... -1i*k*layerRI(length(layerRI))*... exp(-1i*k*layerRI(length(layerRI))*xCurrent)... -1i*k*1*exp(1i*k*1*xCurrent)]; %Defining column matrix containing the array of free %terms. %Nonzero elements of this array are only two first %elements because we assumed A0 to be equal to 1. For %all other equations free terms equal to zero freeMemberMatrix=zeros(length(layerWidth)*2+2,1); freeMemberMatrix(1)=-1; freeMemberMatrix(2)=-1*1i*k*1; %Cycle for Cramer’s method solution %Cashing the matrix to some temporary variable.

3. In which case does the Fresnel reflection appear? 4. Derive Helmholtz equation for magnetic field. 5. Derive the Helmholtz equation for electric field for the medium with magnetic and dielectric properties (μ = μ(r), ε = ε(r)). 6. Derive the Helmholtz equation for magnetic field for the medium with magnetic properties only (μ = μ(r), ε = const). 7. By solving Helmholtz equation for electric field and nonmagnetic medium, derive the formula for Fresnel reflection from one interface: R = (n1 − n2 )/(n1 + n2 ).

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Photonic Crystals: Physics and Practical Modeling by Igor A. Sukhoivanov


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