TM wave

[¦tē′em ‚wāv]

(electromagnetism)

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introduced nonconforming UPML theory into DG calculations in the case of TM wave and compared the local relative error between PML and first-order SM-ABC [14].

Implementation of an Approximate Conformal UPML in 2-D DGTD

From (9) and (25), the TM wave equation in the beam region can be obtained as

Electromagnetic Waves Dispersion and Interaction of an Annular Beam-Ion Channel System in Plasma Waveguide

Smol'kin, "Method of cauchy problem to solve a nonlinear transmission eigenvalue problem for tm wave propagating in a circle double-layer dielectric waveguide with kerr nonlinearity," Izvestiya Vysshikh Uchebnykh Zavedenij.

Nonlinear double-layer Bragg waveguide: analytical and numerical approaches to investigate waveguiding problem

The above formulations can be applied to TM wave by simple replacements of [p.sub.i], [p.sub.0], and [p.sub.s] as follows:

Properties of the band gaps in 1D ternary lossy photonic crystal containing double-negative materials

Since biaxial anisotropic medium is a reciprocal medium, if total transmission occurs at the boundary when a TM wave is incident from isotropic medium into biaxial anisotropic medium, total transmission will also occur when this TM wave is incident from biaxial anisotropic medium into the same isotropic medium.

A Wave Splitter with Simple Structure Based on Biaxial Anisotropic Medium

Analogous derivations for TM wave result in a similar formula with [E.sub.[phi]] replaced with [H.sub.[phi]] and [H.sub.[phi]] replaced with [-E.sub.[phi]] which is the consequence of the natural symmetry of Maxwell equations.

The currents induced by a high-frequency wave incident at a small angle to the axis of strongly elongated spheroid

where coefficients [q.sub.i,s] = [n.sub.i,s]cos[[theta].sub.j,s] for the TE wave and coefficients [q.sub.i,s] = cos[[theta].sub.j,s] / [n.sub.i,s] for the TM wave, where the subscripts i, j and s correspond to the quantities in the incident medium, periodic medium of photonic crystal and substrate respectively.

Tunable multi-channel filtering using 1-D photonic quantum well structures

For two-dimensional electromagnetic scattering problems, rectangular components of the electromagnetic field may be classified as independent groups, namely, TM wave and TE wave.

Electromagnetic Scattering by Multiple Columns Partially Buried in a Ground Plane

Similarly, for the induced current of the TM wave, we get

Recent Advances in the Asymptotic Theory of Diffraction by Elongated Bodies

The above calculations can be used for TM wave by substituting [p.sub.l] = cos [[theta].sub.l]/[n.sub.l] where l = 0, 1, 2 and 3.

Characterization of defect modes in one-dimensional ternary metallo-dielectric nanolayered photonic crystal

Consider a TM wave incident from air (z < 0) to the metamaterial slab (z > 0), such that the total, incident, and reflected magnetic fields at z < 0 are given by

Effective material property extraction of a metamaterial by taking boundary effects into account at TE/TM polarized incidence

Simulated absorption values at the resonances for TE and TM waves. Angle TE Wave TM Wave (degrees) First Second First Second 0[degrees] 98.46% 99.91% 98.46% 99.89% 15[degrees] 98.49% 99.81% 98.58% 99.88% 30[degrees] 98.56% 99.93% 98.52% 99.65% 45[degrees] 98.51% 99.96% 98.50% 99.93% 60[degrees] 98.45% 99.97% 98.53% 99.94% 75[degrees] 98.47% 99.72% 98.56% 99.90% 90[degrees] 98.37% 99.91% 98.41% 99.94%

Design of Polarization and Incident Angle Insensitive Dual-Band Metamaterial Absorber Based on Isotropic Resonator