Compared to single-mode VCSELs, multimode VCSELs have not received much attention in models and characterizations for functional parameters, despite making up the majority of commercially available VCSELs [1]. In particular, the extraction of the linewidth enhancement factor for multimode VCSELs has been overlooked, likely due to difficulties in measurement. Additionally, multimode models for VCSELs have, until recently, omitted spectral characteristics such as linewidth [2]. This is the first work to report a measured linewidth enhancement factor value (lower bound) for a multimode VCSEL. A characterization for the functional parameters of a red multimode vertical-cavity surface-emitting laser (VCSEL) is shown herein. The extracted values form a complete working set of parameters for the laser rate equations. The techniques employed for extracting values include frequency responses, power versus current fittings, and optical spectral measurements. From the frequency responses at various bias currents, the relaxation oscillation frequency and damping factor are found. The power versus current curve is fitted to find parameters including the modal spontaneous emission rate and carrier density at threshold. The spectral measurements are used for evaluating the linewidth enhancement factor (LEF) also known as the alpha factor or Henry factor. These 5 methods have been applied previously to characterizing single-mode VCSELs [3]–[5]. The experimentally extracted parameters herein are important for creating accurate models and simulations for multimode VCSELs. Improved multimode VCSEL models are necessary for improving optical communication, especially for short-range optical interconnects [2]. The measured parameters for the characterized VCSEL are comparable to similar single-mode VCSELs characterized in other works. This is promising because multi-mode VCSELs have higher output power than their single-mode counterparts, thus these results may aid in improving short-range optical interconnects.

A power system stability is essential for maintaining the power system oscillation frequency within a small and acceptable interval around its nominal frequency. Hence, it is necessary to study and control the frequency for stable operation of a power system by knowing the characteristics within a power system. One approach is to understand the effectiveness of frequency and damping characteristics of generators in power systems. Hence, the simulation analysis of IEEE 118-bus power system is used for this study. The analysis includes theoretical analysis with a mathematical approach and simulation studies of swing equation to determine the characteristics of damped single-machine infinite bus, which is represented as a generator connects to a large network system with a small signal disturbance by line losses. Additionally, mathematical derivation of Prony analysis is presented in order to estimate the frequency and damping ratio of the simulation results. In the end, the results demonstrate that the frequency and damping characteristics of generators are highly dependent on the system inertia constant. Therefore, the higher inertia constant is a critical factor to ensure the system is more stable. / Master of Science

As the thinnest material ever with high carrier mobility and saturation velocity, graphene is considered as a candidate for future high speed electronics. After pioneering research on graphene-based electronics at Georgia Tech, epitaxial graphene on SiC, along with other synthesized graphene, has been extensively investigated for possible applications in high frequency analog circuits. With a combined effort from academic and industrial research institutions, the best cut-off frequency of graphene radio-frequency (RF) transistors is already comparable to the best result of III-V material-based devices. However, the power gain performance of graphene transistors remained low, and the absence of a band gap inhibits the possibility of graphene in digital electronics. Aiming at solving these problems, this thesis will demonstrate the effort toward better high frequency power gain performance based on mono-layer epitaxial graphene on C-face SiC. Besides, a graphene/Si integration scheme will be proposed that utilizes the high speed potential of graphene electronics and logic functionality and maturity of Si-CMOS platform at the same time.

Cette thèse porte sur l’étude théorique de nouveaux concepts de transistors en graphène par le formalisme des fonctions de Green dans l’hypothèse du transport balistique. Le graphène est un matériau bidimensionnel composé d’atomes de carbone organisés en nid d’abeille. Cette structure confère des propriétés uniques aux porteurs de charge dans le graphène, comme une masse effective nulle et un comportement ultra-relativiste (fermions de Dirac), ce qui conduit à des mobilités extraordinairement élevées. C’est pourquoi des efforts très importants ont été mis en œuvre dans la communauté scientifique pour la réalisation de transistors en graphène. Cependant, en vue de nombreuses applications, le graphène souffre de l’absence d’une bande d’énergie interdite. De plus, dans le cas des transistors conventionnels à base de graphène (GFET), cette absence de bande interdite, combinée avec l’apparition de l’effet tunnel de Klein, a pour effet de dégrader considérablement le rapport I_ON/I_OFF des GFET. L’absence de gap empêche également toute saturation du courant dans la branche N – là où se trouve le maximum de transconductance pour des sources et drain dopés N – et ne permet donc pas de tirer profit des très bonnes performances fréquentielles que le graphène est susceptible d’offrir grâce aux très hautes mobilités de ses porteurs. Cependant, de précédents travaux théorique et expérimentaux ont montré que la réalisation d’un super-réseau d’anti-dots dans la feuille de graphène – appelée Graphene NanoMesh (GNM) – permettait d’ouvrir une bande interdite dans le graphène. On s’est donc d’abord proposé d’étudier l’apport de l’introduction de ce type de structure pour former canal des transistors – appelés GNMFET – par rapport aux GFET « conventionnels ». La comparaison des résultats obtenus pour un GNM-FET avec un GFET de mêmes dimensions permettent d’affirmer que l’on peut améliorer le rapport I_ON/I_OFF de 3 ordres de grandeurs pour une taille et une périodicité adéquate des trous. Bien que l’introduction d’un réseau de trous réduise légèrement la fréquence de coupure intrinsèque f_T, il est remarquable de constater que la bonne saturation du courant dans la branche N, qui résulte de la présence de la bande interdite dans le GNM, conduit à une fréquence maximale d’oscillation f_max bien supérieure dans le GNM-FET. Le gain en tension dans ce dernier est aussi amélioré d’un ordre de grandeur de grandeur par rapport au GFET conventionnel. Bien que les résultats sur le GNM-FET soient très encourageants, l’introduction d’une bande interdite dans la feuille de graphène induit inévitablement une masse effective non nulle pour les porteurs, et donc une vitesse de groupe plus faible que dans le graphène intrinsèque. C’est pourquoi, en complément de ce travail, nous avons exploré la possibilité de moduler le courant dans un GFET sans ouvrir de bande interdite dans le graphène. La solution que nous avons proposée consiste à utiliser une grille triangulaire à la place d’une grille rectangulaire. Cette solution exploite les propriétés du type "optique géométrique" des fermions de Dirac dans le graphène, qui sont inhérentes à leur nature « Chirale », pour moduler l’effet tunnel de Klein dans le transistor et bloquer plus efficacement le passage des porteurs dans la branche P quand le dopage des sources et drains sont de type N. C’est pourquoi nous avons choisi d’appeler ce transistor le « Klein Tunneling FET » (KTFET). Nous avons pu montrer que cette géométrie permettrait d’obtenir un courant I_off plus faible que ce qui est obtenu d’habitude, pour la même surface de grille, pour les GFET conventionnels. Cela offre la perspective d’une nouvelle approche de conception de dispositifs permettant d’exploiter pleinement le caractère de fermions de Dirac des porteurs de charges dans le graphène. / This thesis is a theoretical study of new concepts of graphene-based transistors using non equilibrium Green’s function formalism in the ballistic limit. Graphene is a two-dimensional material made of a honeycomb arrangement of carbon atoms. This crystallographic structure allows electrons to behave like ultra-relativistic particles, namely massless Dirac fermions. This yields extraordinary high mobility for charge carriers in this material and a huge potential for high frequency applications. Consequently, strong efforts have been made in the scientific community towards the implementation of this material as a channel for field effect transistors. Unfortunately, graphene suffers from the lack of an energy band gap, and the Klein tunneling effect that takes place in Graphene Field Effect Transistor’s (GFET) channel makes it impossible to back-scatter completely the carriers even for high potential barriers. This degrades considerably the I_ON/I_OFF ratio obtained in GFETs. Additionally, the absence of a band gap makes it impossible to obtain current saturation in the N branch, where the maximum of transconductance is reached for n-doped source and drain regions, preventing to take full advantage from the huge potential for high frequency application of graphene. Fortunately, it has been demonstrated in both theoretical and experimental works that Graphene NanoMesh (GNM), a structure obtained after punching an anti-dot super-lattice in the graphene sheet, can open a band gap for charge carriers. This has motivated our study of a field effect transistor where the GNM is used as a channel (GNMFET) and to compare its performance with the conventional GFET. Our study showed that the use of this type of transistors can improve the I_ON/I_OFF ratio up to 3 orders of magnitude when the GNM is carefully chosen. Though the introduction of the anti-dots in the graphene sheet reduces the transit frequency f_T, it is remarkable that the good saturation that occurs in the N branch, as a result of the band gap opening, yields a much higher maximum oscillation frequency f_max in the GNMFET. The voltage gain is also improved by an order of magnitude compared to its GFET counterpart. Though the performance of the GNMFET is very encouraging, the band gap opening in the GNM confers a finite effective mass to the carriers in graphene, resulting in lower group velocity compared to the case of pristine graphene. This is why we explored a new solution that avoids the band gap opening to modulate the current in graphene-based transistors. We proposed the use of a triangular gate of the transistor. The operation of this transistor relies on optics-like behavior of Dirac fermions that emerges from their “chiral” properties, giving the possibility to modulate the Klein tunneling. We called this transistor the “Klein Tunneling Field Effect Transistor” (KTFET), and we showed that that this prismatic gate shape enables the KTFET to have an “OFF” current I_OFF that is lower than the one that it obtained for the conventional GFET and which is determined by the Dirac point. This study paves the way for a new approach to designing graphene devices which fully exploits the Dirac fermions nature of particles in graphene.