Search arXivSearch

arXiv · 2401.14812

Design and simulation of highly selective graphene-silicon nitride integrated dual-mode electro-absorption modulators

Abstract

We present the design, simulation and optimization of an integrated graphene-silicon nitride dual-mode modulator with high mode selectivity, optimized for a wavelength of 1.55 $μ$m. The proposed device finds applications in mode division multiplexing systems, enabling the simultaneous and independent switching of two transverse electric modes supported by a buried dual-mode silicon nitride waveguide (TE$_0$ and TE$_1$). Three graphene-Al$_2$O$_3$-graphene nanoribbons are integrated on top of the waveguide. A central nanoribbon acts as a TE$_0$ mode absorber, while the two remaining nanoribbons located on the sides act as TE$_1$ mode absorbers. Their absorption is tuned by modifying the Fermi energy of graphene, which can be achieved through electrical doping. Thus, the corresponding nanoribbons operate as selective TE$_0$ and TE$_1$ modulators with a total energy consumption per unit length under 2430 pJ bit$^{-1}$ cm$^{-1}$. The modulation depth of each mode can reach up to 316 dB/cm and 273 dB/cm, respectively, while maintaining a selection ratio of 5.63$-$6.28 and extinction ratio of 204$-$248 dB/cm between them. Under thinner Al$_2$O$_3$ conditions, consumption below 607.5 pJ bit$^{-1}$ cm$^{-1}$ can be achieved with a marginal reduction of the optical performance in the TE$_1$ modulator. Overall, we report the design of a fully optimized integrated dual-mode modulator based on graphene tunable electro-absorption, opening the path toward integrated efficient multimode optical communication systems.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

Fernando Martín-Romero, Víctor Jesús Gómez. 2026-09-10. Design and simulation of highly selective graphene-silicon nitride integrated dual-mode electro-absorption modulators. https://arxiv.org/abs/2401.14812

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

RCS angular control with gradient metasurfaces: design and measurement

This letter proposes the design and measurement of a periodic metasurface that achieves anomalous reflection with reduced RCS in a given parasitic direction. A previous study proposed a semi-analytical model to predict the RCS behavior of such a metasurface. However, this first study did not include any experimental exploration to verify the theoretical results. To complete this study, this work presents an experimental validation of the proposed design, with a focus on manufacturing and measurement issues. The synthesis, design specifications, fabrication method and experimental setup are presented and discussed. Measurement results are also examined in detail, highlighting some limitations in metasurfaces RCS measurements. The proposed metasurface effectively achieves the predicted RCS level reduction in the considered parasitic direction. The agreement between simulation and experimental results demonstrates the accuracy of the modelling and the efficiency of the optimisation procedure.

physics.app-ph

Maximum-Power-Transfer Power Coordinates for Fully Coupled Multiport Thévenin Sources

A power-normalized scattering representation is developed at a fixed frequency for a passive linear time-invariant multiport load driven by a fully coupled multiport Thévenin source. The source is obtained by reducing, at the load reference planes, an independent-source network whose suppressed internal impedance is passive, together with an intervening passive matching network. No diagonal-reference, uncoupled-source-channel, reciprocity, or commutation assumption is required. With $R_s=\mathrm{Herm}\{Z_s\}\succ\mathbf{0}$, completing the square in accepted power identifies the available-power current and motivates the coordinates $\mathbf{a}=\frac12R_s^{-1/2}(\mathbf{V}+Z_s\mathbf{I})$, $\mathbf{b}=\frac12R_s^{-1/2}(\mathbf{V}-Z_s^H\mathbf{I})$. They satisfy $\|\mathbf{a}\|_2^2-\|\mathbf{b}\|_2^2=\Re\{\mathbf{I}^H\mathbf{V}\}$ and yield $\mathbf{S}=R_s^{-1/2}(Z_{load}-Z_s^H)(Z_{load}+Z_s)^{-1}R_s^{1/2}$. An exact operator identity establishes passivity--contractivity equivalence and gives excitation-specific, reachable-subspace, and complete conjugate-matching conditions. On the physically reachable incident subspace, singular values characterize the best- and worst-case source-normalized port-reflection TARC, while a restricted Frobenius norm gives the basis-averaged squared TARC. Equal-magnitude phase-only control is formulated separately as a constant-modulus problem, with generator-side constraints mapped through the coupled source network before power normalization. For antenna loads and excitations with $P_{acc}>0$, $P_{rad}/P_{av}=η_{rad}(1-\mathrm{TARC}^2)$, so terminal scattering data alone do not determine radiation efficiency. When $R_s$ is singular, finite available power exists exactly for $\mathbf{E}\in\mathrm{range}(R_s)$, and the construction applies on the positive-resistance support.

physics.app-ph

Bimorph Lithium Niobate Thickness-Shear Overtone Film Bulk Acoustic Resonator

High quality factor ($Q$) and overtone operation enable narrow-linewidth acoustic devices with multiple discrete frequencies in a single cavity. Maintaining both high $Q$ and sufficient electromechanical coupling at higher mode orders remains challenging. Here, we demonstrate a bimorph periodically poled piezoelectric film (P3F) lithium niobate (LN) platform for high-order thickness-shear (TS) overtone excitation. The device comprises a bonded 80-$μ$m-thick single-crystal X-cut LN bimorph with opposite polarizations, patterned top and floating bottom electrodes, and a suspended air cavity. The P3F configuration mitigates charge cancellation from the alternating stress distribution of higher-order TS modes, enabling measurable coupling across a broad sequence of overtones. The thick LN acoustic cavity and increasingly confined high-order mode profiles support low-loss operation. Measured TS overtones extend to 1.75 GHz. At room temperature, representative overtones at 0.77 and 0.89 GHz exhibit 3-dB $Q$ values of 11,338 and 11,917, corresponding to $fQ$ products of $8.74\times10^{12}$ and $1.06\times10^{13}$ Hz, respectively. Cooling from 297 to 12 K systematically enhances $Q$, yielding a peak 3-dB $Q$ of 20,507 at 779 MHz and a maximum $fQ$ product of $1.98\times10^{13}$ Hz at 1.379 GHz. These results establish bimorph P3F LN as a promising platform for high-$Q$, frequency-scalable micro-acoustic resonators in the sub-GHz and low-GHz regimes.

physics.app-ph