Dynamically controllable, homogeneous, anisotropic metamaterials with simultaneous attenuation and amplification

Abstract

Anisotropic homogeneous metamaterials that are neither wholly dissipative nor wholly active at a specific frequency are permitted by classical electromagnetic theory. Well-established homogenization formalisms indicate that such a metamaterial may be realized quite simply as a random mixture of electrically small (possibly nanoscale) spheroidal particles of at least two different isotropic dielectric materials, one of which must be dissipative but the other active. The dielectric properties of this metamaterial are influenced by the volume fraction, spatial distribution, particle shape and size, and the relative permittivities of the component materials. Similar metamaterials with more complicated linear as well as nonlinear constitutive properties are possible. Dynamic control of the active component material, for example via stimulated Raman scattering, affords dynamic control of the metamaterial.

Cited by in corpus (8)

• Surface-Wave Propagation on Non-Hermitian Metasurfaces with Extreme Anisotropy
• On Dyakonov-Voigt surface waves guided by the planar interface of dissipative materials
• Voigt-wave propagation in active materials
• Polarization-state-dependent attenuation and amplification in a columnar thin film
• Simultaneous amplification and attenuation in isotropic chiral materials
• Electromagnetic surface waves guided by the planar interface of isotropic chiral materials
• On electromagnetic surface waves supported by an isotropic chiral material
• Simultaneous existence of amplified and attenuated Dyakonov surface waves