Afin de dépasser la limite d'échelle, il existe une solution innovante qui permet de fabriquer des structures multi-grilles. Ainsi, un NMOSFET composé de trois grilles indépendantes fabriquées dans la technologie CMOS. En dehors de leur forme, géométrique, le transistor multi-grille est similaire à une structure classique. Une multi-grille NMOSFET peut être fabriquée par l'intégration de tranchées de polysilicium. Ces tranchées sont utilisées dans diverses applications telles que les mémoires DRAM, électronique de puissance ou de capteurs d'image. Les capteurs d'image présentent le problème des charges parasites entre les pixels, appelées diaphonie. Les tranchées sont l'une des solutions qui réduisent ce phénomène. Ces tranchées assurent l'isolation électrique sur toute la matrice des pixels. Nous avons étudié ses caractéristiques en utilisant des mesures I-V, méthode du split C-V et de pompage de charge à deux et à trois niveaux. Son multi-seuil caractéristique a été vérifié. Nous n'avons observé aucune dégradation significative de ces caractéristiques grâce à l'intégration des tranchées. La structure a été simulée par la méthode des éléments finis en 3D via le logiciel TCAD. Ses caractéristiques électriques ont été simulées et confrontées avec les résultats obtenus à partir de mesures électriques. La tension de seuil et la longueur de canal effective ont été extraites. Sa mobilité effective et les pièges de l'interface Si/SiO2 ont également été simulés ou calculés. En raison des performances électriques satisfaisantes et d'un bon rendement, nous avons remarqué que ce dispositif est une solution adéquate pour les applications analogiques grâce aux niveaux de tension multi-seuil / One of the recent solutions to overcome the scaling limit issue are multi-gate structures. One cost-effective approach is a three-independent-gate NMOSFET fabricated in a standard bulk CMOS process. Apart from their shape, which takes advantage of the three-dimensional space, multi gate transistors are similar to the conventional one. A multi-gate NMOSFET in bulk CMOS process can be fabricated by integration of polysilicon-filled trenches. This trenches are variety of the applications for instance in DRAM memories, power electronics and in image sensors. The image sensors suffer from the parasitic charges between the pixels, called crosstalk. The polysilicon - filled trenches are one of the solution to reduce this phenomenon. These trenches ensure the electrical insulation on the whole matrix pixels. We have investigated its characteristics using l-V measurements, C-V split method and both two- and three-level charge pumping techniques. Tts tunable-threshold and multi-threshold features were verified. Tts surface- channel low-field electron mobility and the Si/SiO2 interface traps were also evaluated. We observed no significant degradation of these characteristics due to integration of polysilicon-filled trenches in the CMOS process. The structure has been simulated by using 3D TCAD tool. Tts electrical characteristics has been evaluated and compared with results obtained from electrical measurements. The threshold voltage and the effective channel length were extracted. Tts surface-channel low-field electron mobility and the Si/SiO2 interface traps were also evaluated. Owing to the good electrical performances and cost-effective production, we noticed that this device is a good aspirant for analog applications thanks to the multi-threshold voltages

Les capteurs d'images CMOS ont connu au cours des six dernières années une réduction de la taille des pixels d'un facteur quatre. Néanmoins, cette miniaturisation se heurte à la diminution rapide du signal maximal de chaque pixel et à l'échange parasite entre pixels (diaphotie). C'est dans ce contexte qu'a été développé le Pixel à Tranchées Profondes Capacitives et Grille de Transfert verticale (pixel CDTI+VTG). Basé sur la structure d'un pixel « 4T », il intègre une isolation électrique par tranchées, une photodiode profonde plus volumineuse et une grille verticale permettant le stockage profond et le transfert des électrons. Des procédés de fabrication permettant cette intégration spécifique ont tout d'abord été développés. Parallèlement, une étude détaillée des transistors du pixel, également isolés par CDTI a été menée. Ces tranchées capacitives d'isolation actionnées en tant que grilles supplémentaires ouvrent de nombreuses applications pour un transistor multi-grille compatible avec un substrat massif. Un démonstrateur de 3MPixels intégrant des pixels d'une taille de 1.75*1.75 μm² a été réalisé dans une technologie CMOS 120 nm. Les performances de ce capteur ont pu être déterminées, en particulier en fonction de la tension appliquée aux CDTI. Un bas niveau de courant d'obscurité a tout particulièrement été obtenu grâce à la polarisation électrostatique des tranchées d'isolation / CMOS image sensors showed in the last few years a dramatic reduction of pixel pitch. However pitch shrinking is increasingly facing crosstalk and reduction of pixel signal, and new architectures are now needed to overcome those limitations. Our pixel with Capacitive Deep Trench Isolation and Vertical Transfer Gate (CDTI+VTG) has been developed in this context. Innovative integration of polysilicon-filled deep trenches allows high-quality pixel isolation, vertically extended photodiode and deep vertical transfer ability. First, specific process steps have been developed. In parallel, a thorough study of pixel MOS transistors has been carried out. We showed that capacitive trenches can be also operated as extra lateral gates, which opens promising applications for a multi-gate transistor compatible with CMOS-bulk technology. Finally, a 3MPixel demonstrator integrating 1.75*1.75 μm² pixels has been realized in a CMOS 120 nm technology. Pixel performances could be measured and exploited. In particular, a low dark current level could be obtained thanks to electrostatic effect of capacitive isolation trenches

Undoped body multi gate (MG) Metal Oxide Semiconductor Field Effect Transistors (MOSFET) are appearing as replacements for single gate bulk MOSFET in forthcoming sub-45nm technology nodes. It is therefore extremely necessary to develop compact models for MG transistors in order to use them in nano-scale integrated circuit design and simulation. There is however a sharp distinction between the electrostatics of traditional bulk transistors and undoped body devices. In bulk transistor, where the substrate is sufficiently doped, the inversion charges are located close to the surface and hence the surface potential solely controls the electrostatic integrity of the device. However, in undoped body devices, gate electric field penetrates the body center, and inversion charge exists throughout the body. In contrast to the bulk transistors, depending on device geometry, the potential of the body center of undoped body devices could be higher than the surface in weak inversion regime and the current flows through the center-part of the device instead of surface. Several crucial parameters (e.g. Sub-threshold slope) sometimes become more dependable on the potential of body center rather than the surface. Hence the body-center potential should also be modeled correctly along with the surface-potential for accurate calculation of inversion charge, threshold voltage and other related parameters of undoped body multi-gate transistors. Although several potential models for MG transistors have been proposed to capture the short channel behavior in the subthreshold regime but most of them are based on the crucial approximation of coverting the 2D Poisson’s equation into Laplace equation. This approximation holds good only at surface but breaks down at body center and in the moderate inversion regime. As a result all the previous models fail to capture the potential of body center Correctly and remain valid only in weak-inversion regime. In this work we have developed semiclassical compact models for potential distribution for double gate (DG) and cylindrical Gate-All-Around (GAA) transistors. The models are based on the analytical solution of 2D Poisson’s equation in the channel region and valid for both: a) weak and strong inversion regimes, b) long channel and short channel transistors, and, c) body surface and center. Using the proposed model, for the first time, it is demonstrated that the body potential versus gate voltage characteristics for the devices having equal channel lengths but different body thicknesses pass through a single common point (termed as crossover point). Using the concept of “crossover point” the effect of body thickness on the threshold voltage of undoped body multi-gate transistors is explained. Based on the proposed body potential model, a new compact model for the subthreshold swing is formulated. Some other parameters e.g. inversion charge, threshold voltage roll-off etc are also studied to demonstrate the impact of body center potential on the electrostatics of multi gate transistor. All the models are validated against professional numerical device simulator.