% IMPORTANT: The following is UTF-8 encoded. This means that in the presence % of non-ASCII characters, it will not work with BibTeX 0.99 or older. % Instead, you should use an up-to-date BibTeX implementation like “bibtex8” or % “biber”. @PHDTHESIS{Noei:794157, author = {Noei, Maziar}, othercontributors = {Jungemann, Christoph and Meinerzhagen, Bernd}, title = {{D}eterministic simulation of junctionless nanowire field effect transistors}, school = {Rheinisch-Westfälische Technische Hochschule Aachen}, type = {Dissertation}, address = {Aachen}, reportid = {RWTH-2020-07441}, pages = {1 Online-Ressource (148 Seiten) : Illustrationen, Diagramme}, year = {2020}, note = {Veröffentlicht auf dem Publikationsserver der RWTH Aachen University; Dissertation, Rheinisch-Westfälische Technische Hochschule Aachen, 2020}, abstract = {As the feature lengths of the field-effect transistors (FETs) are scaled down to the deca-nanometer range, the commonly used macroscopic approaches such as drift-diffusion and hydrodynamic models lose their validity and a detailed description of the microscopic behavior of charge carriers becomes essential for device simulation. In this work, a fully self-consistent and deterministic solver for the system of Poisson, Schrödinger, and Boltzmann equations tailored to the specific case of gate-all-around junctionless nanowire FETs is developed. The simulation framework employs various numerical techniques such as the H-transformation and an even/odd decomposition of the distribution function on a staggered grid for stabilization of the Boltzmann equation (BE), and the equations are solved with the Newton-Raphson approach which demonstrates quadratic convergence within just a few iterations. Different inter- and intra-valley scattering mechanisms, suitable boundary conditions, and quantization effects are included, and the solver is shown to be robust and stable even in the deep subthreshold region. In addition to the stationary simulations, small signal analysis is carried out under the sinusoidal steady state condition and important figures of merit such as the cut-off frequency, maximum oscillation frequency, and Rollet stability factor are obtained and discussed. Moreover, the Langevin-source approach is used for self-consistent calculation of noise, resulting in the first deterministic BE solver for noise analysis of nanowire FETs. Quantities such as the power spectral densities of terminal currents, the drain and gate excess noise factors, cross-correlation, and the noise suppression factors are presented and compared for different gate lengths. In the second part of this work, an alternative approach based on the characteristic curves and matrix exponentials is developed for the discretization of the BE, which is also applicable to the ballistic transport and does not sufferfrom the numerical deficiencies of H-transformation in 1D phase space. The results of the quasi-ballistic simulations are presented and compared to those of the moments equations obtained from the projection of the BE onto Hermite polynomials. It is shown that the predominantly ballistic phenomena cannot be treated with systems of moments equations and simplified boundary conditions. The failure of moments model in describing the ballistic modes of transport has important implications for the existence of Dyakonov-Shur terahertz instabilities in high mobility 1D devices.}, cin = {611410}, ddc = {621.3}, cid = {$I:(DE-82)611410_20140620$}, typ = {PUB:(DE-HGF)11}, doi = {10.18154/RWTH-2020-07441}, url = {https://publications.rwth-aachen.de/record/794157}, }