IEEE Transactions on Electron Devices · 1987 · 122 citations · 20 references
Natural SciencesMaterials EngineeringMaterials ScienceElectronic MaterialsInterface ScienceSemiconductor MaterialsInterface EngineeringOxide SemiconductorsAnnealingNitridationNitride Thin FilmsRapid Thermal AnnealingSecondary Ion Mass SpectrometrySilicon NitrideThermal AnnealingThin-film Oxides
Ultrathin oxides (5-12 nm) were nitrided by lamp-heated rapid thermal annealing in ammonia at temperatures of 900-1150°C for 5-300 s. Elemental depth profiles were measured by Auger electron spectroscopy (AES) and secondary ion mass spectroscopy (SIMS). Both the nitrogen concentration measured by AES and the hydrogen one measured by SIMS for a nitrided oxide are found to increase monotonically as nitridation proceeds. The AES depth profiles of oxygen show that the Si-SiO <inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</inf> interface does not move during nitridation. Dependences of midgap interface state density ( <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">D_{it}_{m}</tex> ) and fixed charge density (N <inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">f</inf> ) on nitridation temperature and on oxide thickness were studied. For a given temperature, both <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">D_{it}_{m}</tex> and (N <inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">f</inf> ) are found to show turnarounds as nitridation time increases in a similar manner: at first both increase, reach respective maxima at a certain nitridation time <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">t_{\max}</tex> , and then decrease gradually. The ( <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">D_{it}_{m}</tex> ) and (N <inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">f</inf> ) increase more rapidly and the <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">t_{\max}</tex> is shorter as the nitridation temperature is raised or the oxide film is thinner. The maximum of <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">D_{it}_{m}</tex> increases as the oxide film is thinner. A two-step model is newly proposed to explain the turn-around behaviors of <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">D_{it}_{m}</tex> and N <inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">f</inf> : the first step is defect formation as a result of nitrogen incorporation and the second step is reduction of the defects by an annealing-type process. The simulation reproduces the turnaround behaviors very well.
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Physics of Semiconductor Devices
Samarth Jain, S. Radhakrishna · 1987 · 4.2K citations
Radiation effects in nitrided oxides
Fred L. Terry, Richard Aucoin, M. Naiman et al. · IEEE Electron Device Letters · 1983 · 127 citations
R. P. Vasquez, A. Madhukar · Applied Physics Letters · 1985 · 112 citations