Polarization is one of the basic properties of electromagnetic waves conveying valuable information in signal transmission and sensitive measurements. Conventional methods for advanced polarization control impose demanding requirements on material properties and attain only limited performance. We demonstrated ultrathin, broadband, and highly efficient metamaterial-based terahertz polarization converters that are capable of rotating a linear polarization state into its orthogonal one. On the basis of these results, we created metamaterial structures capable of realizing near-perfect anomalous refraction. Our work opens new opportunities for creating high-performance photonic devices and enables emergent metamaterial functionalities for applications in the technologically difficult terahertz-frequency regime.

We present the design, numerical simulations and experimental measurements of THz metamaterial absorbers with a broad and flat absorption top both for transverse electric and transverse magnetic polarizations over a wide incidence angle range. The metamaterial absorber unit cell consists of two sets of structures resonating at different but close frequencies. The overall absorption spectrum is the superposition of individual components and becomes flat at the top over a significant bandwidth. The experimental results are in excellent agreement with numerical simulations. c 2018 Optical Society of America OCIS codes: 160.3918, 230.3990, 300.6495, 310.3915 Since the first demonstration by Landy et al.[1], metamaterial absorbers have attracted a great deal of interest worldwide during the past few years due to a host of potential applications including detectors, imaging, and sensing. They are typically comprised two structured metallic layers separated with a dielectric spacer, either free standing or supported by a suitable substrate, with a total thickness of functional layers much smaller than the operational wavelength. The originally proposed bottom structured metallic layer was a resonant cut-wire array [1,2], which has evolved to a simpler metal ground plane [3]. This makes the metamaterial absorbers more or less resemble Salisbury screens or circuit analog absorbers [4]. A variety of metamaterial structures have been employed and the operational frequency has covered the microwave [1] through terahertz (THz) [2, 3, 5] to optical [6, 7] ranges. The generally accepted idea was that by tuning the effective electric permittivity ǫ and magnetic permeability µ independently, it is possible to realize impedance matching to free-space [1] and minimize the reflection. However, it has been recently found that a Fabry-Perót resonance between the two metallic layers is responsible for the observed metamaterial absorption [8], where the tuned reflection/transmission amplitude and phase by the metamaterial layers satisfy the antireflection requirements similar to a quarter wave antireflection, i.e. another kind of impedance matching. We have verified this mechanism for many metamaterial absorbers proposed in literature [9]. Besides its polarization and incidence angle dependence, the bandwidth of a metamaterial absorber is one of the important aspects that may affect many applications. So far, most designs of metamaterial absorbers operate at a specific narrow frequency range. and triple-band [13, 14] metamaterial absorbers have been demonstrated with distinct narrow absorption frequencies; however, broadband metamaterial absorbers remain a challenge and there have been only a few very recent studies, mostly focusing on theoretical and numerical investigation [15][16][17][18][19][20]. In this Letter, we experimentally demonstrate metamaterial absorbers operating in the THz frequency range with a broad and flat high absorption top over a wide incidence angle range, which are in excellent agreement with numerical ...

We investigate the impact of resonator geometry and its coupling with ground plane on the performance of metamaterial perfect absorbers. Using a cross-resonator as an example structure, we find that the absorber thickness can be further reduced through modifying the geometric dimensions of the resonators. Numerical simulations and theoretical calculations reveal that destructive interference of multiple reflections is responsible for the near-unity absorption. The near-field coupling between the resonator array and ground plane can be significant. When this coupling is taken into account, the theoretical results calculated using the interference model are in excellent agreement with experiments and numerical simulations.