Abstract:Two-dimensional transition metal dichalcogenides (2D
TMDCs) are
promising candidates for ultrathin active nanophotonic elements due
to the strong tunable excitonic resonances that dominate their optical
response. Here, we demonstrate dynamic beam steering by an active
van der Waals metasurface that leverages large complex refractive
index tunability near excitonic resonances in monolayer molybdenum
diselenide (MoSe2). Through varying the radiative and nonradiative
rates of the excitons, we can dynamically cont… Show more
“…In particular, electrical gating, optical pumping, thermal annealing, and current-induced heating can be employed for this purpose 14 – 19 Thus far, quantum-confined Stark effects in multiple quantum wells, 20 , 21 molecular phase transitions in vanadium dioxide (VO2) or germanium antimony telluride, 22 reorientation of molecules in liquid crystals, 23 ionic transparent, and carrier-induced field effects in semiconductors, i.e., silicon (Si), gallium arsenide, 24 , 25 transparent conducting oxides (TCOs), 26 – 30 indium arsenide (InAs), 31 , 32 and atomically thin transition metal dichalcogenides, 33 , 34 have been leveraged for index modulation. Among these tuning mechanisms, the free-carrier-induced effects in doped semiconductors have yielded great promise for active tuning thanks to higher modulation frequencies (up to several gigahertz), continuous tunability, and lower power consumption compared to techniques based on the Pockels effect or waveguide modulators based on lithium niobate.…”
.Space–time metasurfaces are promising candidates for breaking Lorentz reciprocity, which constrains light propagation in numerous practical applications. There is a substantial difference between carrier and modulation frequencies in space–time photonic metasurfaces that leads to negligible spatial pathway variation of light and weak nonreciprocal response. To surmount this obstacle, herein, the design principle of a high-quality-factor space–time gradient metasurface is demonstrated at the near-infrared regime that increases the lifetime of photons and allows for strong power isolation by lifting the adiabaticity of modulation. The all-dielectric metasurface consists of an array of silicon subwavelength gratings (SWGs) that are separated from distributed Bragg reflectors by a silica buffer. The resonant mode with ultrahigh quality-factor exceeding 104 is excited within the SWG, which is characterized as magnetic octupole and features strong field localization. The SWGs are configured as multijunction p–n layers, whose multigate biasing with time-varying waveforms enables modulation of carriers in space and time. The proposed nonreciprocal metasurface is exploited for free-space optical power isolation by virtue of modulation-induced phase shift. It is shown that under time reversal and by interchanging the directions of incident and observation ports, power isolation of ≈35 dB can be maintained between the two ports in free space.
“…In particular, electrical gating, optical pumping, thermal annealing, and current-induced heating can be employed for this purpose 14 – 19 Thus far, quantum-confined Stark effects in multiple quantum wells, 20 , 21 molecular phase transitions in vanadium dioxide (VO2) or germanium antimony telluride, 22 reorientation of molecules in liquid crystals, 23 ionic transparent, and carrier-induced field effects in semiconductors, i.e., silicon (Si), gallium arsenide, 24 , 25 transparent conducting oxides (TCOs), 26 – 30 indium arsenide (InAs), 31 , 32 and atomically thin transition metal dichalcogenides, 33 , 34 have been leveraged for index modulation. Among these tuning mechanisms, the free-carrier-induced effects in doped semiconductors have yielded great promise for active tuning thanks to higher modulation frequencies (up to several gigahertz), continuous tunability, and lower power consumption compared to techniques based on the Pockels effect or waveguide modulators based on lithium niobate.…”
.Space–time metasurfaces are promising candidates for breaking Lorentz reciprocity, which constrains light propagation in numerous practical applications. There is a substantial difference between carrier and modulation frequencies in space–time photonic metasurfaces that leads to negligible spatial pathway variation of light and weak nonreciprocal response. To surmount this obstacle, herein, the design principle of a high-quality-factor space–time gradient metasurface is demonstrated at the near-infrared regime that increases the lifetime of photons and allows for strong power isolation by lifting the adiabaticity of modulation. The all-dielectric metasurface consists of an array of silicon subwavelength gratings (SWGs) that are separated from distributed Bragg reflectors by a silica buffer. The resonant mode with ultrahigh quality-factor exceeding 104 is excited within the SWG, which is characterized as magnetic octupole and features strong field localization. The SWGs are configured as multijunction p–n layers, whose multigate biasing with time-varying waveforms enables modulation of carriers in space and time. The proposed nonreciprocal metasurface is exploited for free-space optical power isolation by virtue of modulation-induced phase shift. It is shown that under time reversal and by interchanging the directions of incident and observation ports, power isolation of ≈35 dB can be maintained between the two ports in free space.
“…The intrinsic nature of exciton resonances in 2D-TMDs renders their spectral properties most notably dependent on the band structure of the material, as opposed to the geometry, as with plasmon and Mie-resonators. This allows for their facile integration in more complex architectures. , Furthermore, light scattering by these resonances can be largely and reversibly manipulated via electrostatic free carrier injection, − temperature, , strain, − and external fields, enabling actively tunable nanophotonic devices.…”
mentioning
confidence: 99%
“…At the same time, the strong light–matter interaction within a single TMD monolayer poses an intriguing opportunity to realize atomically thin optical elements. In the limit of single layer metasurfaces, the optical function is dictated by the nanopatterned monolayer only, without influences of external (van-der-Waals heterostructure) cavities, , or plasmon resonances in nanopatterned electrodes. , However, to obtain a complex optical functionality such as wavefront shaping by merely nanopatterning the TMD monolayer, the in-plane dimensions of small flakes are typically the limiting factor in achieving the desired functionality. The size obstacle can be resolved by using chemical-vapor deposition (CVD) growth techniques.…”
mentioning
confidence: 99%
“…Following the procedure outlined in ref , we then fit this susceptibility (that was retrieved purely numerically) using a physically meaningful model to extract the excitonic decay rates. We use a constant background term and a Lorentzian oscillator − for each of the ground states of the three main exciton resonances of monolayer WS 2 : χ(E)=χ∞−prefix∑j=A,B,CℏcEj·t·ℏγnormalrj(E−Ej)+iℏγnrj2…”
Monolayer 2D semiconductors, such as WS 2 , exhibit uniquely strong light−matter interactions due to exciton resonances that enable atomically thin optical elements. Similar to geometry-dependent plasmon and Mie resonances, these intrinsic material resonances offer coherent and tunable light scattering. Thus far, the impact of the excitons' temporal dynamics on the performance of such excitonic metasurfaces remains unexplored. Here, we show how the excitonic decay rates dictate the focusing efficiency of an atomically thin lens carved directly out of exfoliated monolayer WS 2 . By isolating the coherent exciton radiation from the incoherent background in the focus of the lens, we obtain a direct measure of the role of exciton radiation in wavefront shaping. Furthermore, we investigate the influence of exciton− phonon scattering by characterizing the focusing efficiency as a function of temperature, demonstrating an increased optical efficiency at cryogenic temperatures. Our results provide valuable insights into the role of excitonic light scattering in 2D nanophotonic devices.
“…As for tunable metasurfaces, various functional materials have been proposed to design metasurfaces, including Ge 2 Sb 2 Te 5 (GST), 20) liquid crystals, 21) InSb, 22) graphene, 23) MoSe 2 24) and so on. It is worth noting that GST has gained significant attention in the NIR regime because of its rapid response, minimal optical losses, excellent stability, and substantial variation in refractive index between its crystalline and amorphous states.…”
Highly precise and controllable focusing of optical vortex beams in the NIR range is essential for applications in biological imaging, nanomanipulation, and other fields. However, achieving tunable vortex beams across a broad spectrum remains a significant challenge. Herein, we propose a varifocal and broadband achromatic metalens capable of effectively correcting chromatic aberration, achieving a maximum focusing efficiency of 40.0% over 1400–1700 nm. Furthermore, through adjustments to the crystalline fraction of Ge2Sb2Te5 (GST), it offers the ability to vary focal lengths from 6.90 to 10.73 μm. This study may further advance NIR communication and imaging systems.
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