Graphene / silicon (G/Si) heterostructures have been studied extensively in the past years for applications as photodiodes, photodetectors and solar cells, with a growing focus on efficiency and performance. Here, a specific contact pattern scheme with interdigitated Schottky and graphene/insulator/silicon (GIS) structures is explored to experimentally demonstrate highly sensitive G/Si photodiodes. With the proposed design, an external quantum efficiency (EQE) of > 80% is achieved for wavelengths ranging from 380 to 930 nm. A maximum EQE of 98% is observed at 850 nm, where the responsivity peaks to 635 mA/W, surpassing conventional Si p-n photodiodes. This efficiency is attributed to the highly effective collection of charge carriers photogenerated in Si under the GIS parts of the diodes. The experimental data is supported by numerical simulations of the diodes. Based on these results, a definition for the ‘true’ active area in G/Si photodiodes is proposed, which may serve towards standardization of G/Si based optoelectronic devices.

Graphene-based devices are planned to augment the functionality of Si and III-V based technology in radio-frequency (RF) electronics. The expectations in designing graphene field-effect transistors (GFETs) with enhanced RF performance have attracted significant experimental efforts, mainly concentrated on achieving high mobility samples. However, little attention has been paid, so far, to the role of the access regions in these devices. Here, we analyse in detail, via numerical simulations, how the GFET transfer response is severely impacted by these regions, showing that they play a significant role in the asymmetric saturated behaviour commonly observed in GFETs. We also investigate how the modulation of the access region conductivity (i.e., by the influence of a back gate) and the presence of imperfections in the graphene layer (e.g., charge puddles) affects the transfer response. The analysis is extended to assess the application of GFETs for RF applications, by evaluating their cut-off frequency.

An analytical model is proposed to determine the potential and the electron concentration in 1D-confined quantum-well structures. This model is applicable to any kind of asymmetric planar device, such as high-electron-mobility transistors or fully depleted semiconductor-on-insulator FETs. It is based on the solution of the Poisson and Schrödinger equations, under the effective mass approximation, for a triangular potential well, and on the first-order perturbation theory. It is grounded on the physics that governs the device operation and avoids the use of any fitting parameter. The analytical solution considers the wave function penetration into the gate insulator, the effective mass discontinuity at the semiconductor-insulator interfaces, and the Fermi-Dirac statistics. Expressions for the calculation of the subband energies, their corresponding wave functions, as well as the potential profile in the structure are provided. It is demonstrated that our analytical model fits very well the numerical results in all operating regimes from subthreshold to strong inversion for different device sizes and materials.

Amorphous indium gallium zinc oxide (a-IGZO) is becoming an increasingly important technological material. Transport in this material is conceptualized as the heavy disorder of the material causing a conduction or mobility band-edge that randomly varies and undulates in space across the entire system. Thus, transport is envisioned as being dominated by percolation physics as carriers traverse this varying band-edge landscape of “hills” and “valleys”. It is then something of a missed opportunity to model such a system using only a compact approach—despite this being the primary focus of the existing literature—as such a system can easily be faithfully reproduced as a true microscopic TCAD model with a real physically varying potential. Thus, in this work, we develop such a “microscopic” TCAD model of a-IGZO and detail a number of key aspects of its implementation. We then demonstrate that it can accurately reproduce experimental results and consider the issue of the addition of non-conducting band-tail states in a numerically efficient manner. Finally, two short studies of 3D effects are undertaken to illustrate the utility of the model: specifically, the cases of variation effects as a function of device size and as a function of surface roughness scattering.

A comprehensive simulation of 2D materials based BioFETs that simultaneously assesses different approaches employed to model the electrolyte-molecule interaction.