Abstract:Structured electromagnetic (EM) waves carrying orbital angular momentum (OAM) have been explored in various frequency regimes to enhance the data capacity of communication systems by multiplexing multiple co-propagating orthogonal OAM beams (i.e., mode-division multiplexing (MDM)). Terahertz (THz) communications in free space have gained interest as THz waves tend to have: (a) larger bandwidth and lower beam divergence than millimeter-waves, and (b) lower interaction with matter conditions than optical waves. … Show more
“…General research on terahertz light, which occupies the 0.1 to 10 THz band of the electromagnetic spectrum, is fuelled by fundamental and practical ramifications in fields as different as biological imaging, [7][8][9] art restoration, [10][11][12] and telecommunications. [13][14][15] Indeed, the nonlinear generation of terahertz pulses from ultrafast optical sources is indeed standard in the field [16][17][18] and it is historically considered a seminal achievement enabling the modern terahertz research area. However, the lack of efficient largearea thin emitters is certainly a fundamental and practical limit, bringing cumbersome experimental setups with complex geometries as well as several other limitations like the resolution limits of novel near-field imaging systems.…”
Metasurfaces represent a new frontier in materials science paving for unprecedented methods of controlling electromagnetic waves, with a range of applications spanning from sensing to imaging and communications. For pulsed terahertz (THz) generation, metasurfaces offer a gateway to tuneable thin emitters that can be utilized for large‐area imaging, microscopy, and spectroscopy. In literature, THz‐emitting metasurfaces generally exhibit high absorption, being based either on metals or on semiconductors excited in highly resonant regimes. Here, the use of a fully dielectric semiconductor exploiting morphology‐mediated resonances and inherent quadratic nonlinear response is proposed. This system exhibits a remarkable 40‐fold efficiency enhancement compared to the unpatterned at the peak of the optimized wavelength range, demonstrating its potential as a scalable emitter design.
“…General research on terahertz light, which occupies the 0.1 to 10 THz band of the electromagnetic spectrum, is fuelled by fundamental and practical ramifications in fields as different as biological imaging, [7][8][9] art restoration, [10][11][12] and telecommunications. [13][14][15] Indeed, the nonlinear generation of terahertz pulses from ultrafast optical sources is indeed standard in the field [16][17][18] and it is historically considered a seminal achievement enabling the modern terahertz research area. However, the lack of efficient largearea thin emitters is certainly a fundamental and practical limit, bringing cumbersome experimental setups with complex geometries as well as several other limitations like the resolution limits of novel near-field imaging systems.…”
Metasurfaces represent a new frontier in materials science paving for unprecedented methods of controlling electromagnetic waves, with a range of applications spanning from sensing to imaging and communications. For pulsed terahertz (THz) generation, metasurfaces offer a gateway to tuneable thin emitters that can be utilized for large‐area imaging, microscopy, and spectroscopy. In literature, THz‐emitting metasurfaces generally exhibit high absorption, being based either on metals or on semiconductors excited in highly resonant regimes. Here, the use of a fully dielectric semiconductor exploiting morphology‐mediated resonances and inherent quadratic nonlinear response is proposed. This system exhibits a remarkable 40‐fold efficiency enhancement compared to the unpatterned at the peak of the optimized wavelength range, demonstrating its potential as a scalable emitter design.
“…Terahertz (THz)-wave technologies have been extensively studied for various applications [1][2][3][4] such as spectroscopic sensing, nondestructive imaging, and telecommunications. For these applications, various THz-wave generation methods have been developed.…”
We propose and numerically investigate integrated photonic crystal waveguides (PhC-WGs) formed in a semiconductor slab to realize an ultrasmall and highly efficient terahertz (THz) wave source. The structure consists of a straight PhC-WG with low-group-velocity and low-dispersion (LVLD) for efficient difference frequency generation (DFG) connected to two PhC-WGs to introduce two fundamental lights into the LVLD PhC-WG. The fundamental light propagating through each PhC-WG designed to enhance their electric fields by the slow-light effect is efficiently coupled to the LVLD PhC-WG owing to the reduced refractive index differences at the boundaries of the heterostructures. The DFG from the two fundamental lights was numerically simulated, and a temporal intensity oscillation corresponding to the difference in frequency was clearly observed. By comparing the DFG intensities of the integrated structures with an LVLD PhC-WG and a strip WG, the estimated DFG intensity from the LVLD PhC-WG was more than 100 times higher than that from the strip WG. These results indicate the effectiveness of the proposed heterostructure in the application of a highly efficient THz source with an ultrasmall footprint compared with conventional materials.
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