The mechanism of the flatband voltage shift by capping a thin layer of Me₂O₃ (Me=Gd, Y and Dy) on SiO₂ and HfO₂-based dielectrics

dc.contributor.advisorLee, Jack Chung-Yeungen
dc.creatorZhang, Manhong, 1969-en
dc.date.accessioned2012-09-21T19:16:22Zen
dc.date.available2012-09-21T19:16:22Zen
dc.date.issued2008-05en
dc.descriptiontexten
dc.description.abstractContinuing to scale down the transistor size makes the introduction of high-k dielectric necessary. However, there are still a lot of problems with highk transistors such as worse reliability and Fermi-level pinning. In HfO₂, low crystallization temperature, fixed charge in the bulk and low quality of the Si/HfO₂ interface cause reliability problems. Fermi-level pinning results in high threshold voltage. For the first work in this dissertation, forming Hf1-xTaxO through doping HfO₂ with Ta is used to improve the crystallization temperature and electron mobility. Then, the fluorine passivation of high-k dielectrics is studied. With fluorine passivation, the electron mobility was improved in NMOSFETs with gate stacks of poly-Si/TaN/HfO₂/p-Si with thin TaN layers. Inserting a 1.5nm layer of HfSiON between TaN and HfO₂ completely blocked the fluorine atoms so that they could not reach the Si interface. Thus, no mobility was improved even with fluorine implantation. In order to decrease threshold voltage, we must study mechanisms of Fermi level pinning (FLP) in high-k gate stacks. We summarize three FLP mechanisms: (1) the dipole formation at the interface between metal gate and high-k dielectric due to hybridization; 2) the dipole formation through oxygen vacancy mechanism; (3) the dipole formation at the interface between high-k dielectric and interfacial SiO₂. The rest of dissertation focuses on the mechanism of Vfb shift by capping a thin layer of Me₂O₃ (Me=Gd, Y and Dy) on SiO₂ and HfO₂-based high-k dielectrics with TaN, W and Pt metal gate. It is proposed that the negative Vfb shift with TaN metal gate be due to the dipole formation at the interface between Me₂O₃ and the interfacial SiO₂. An XPS (X-ray photoelectron spectroscopy) study of Gd₂O₃ capping on SiO₂ indicates clear Si, O and Gd related bonding state change at the interface between Gd₂O₃ (or GdSiO) and the interfacial SiO₂. So the bonding state change is the root cause of the dipole formation. When there is an oxygen deficiency in Me₂O₃, another dipole formation through oxygen vacancy mechanism can also be observed. For a full understanding of the Vfb shift, all three FLP mechanisms must be considered.en
dc.description.departmentElectrical and Computer Engineeringen
dc.format.mediumelectronicen
dc.identifier.urihttp://hdl.handle.net/2152/17971en
dc.language.isoengen
dc.rightsCopyright is held by the author. Presentation of this material on the Libraries' web site by University Libraries, The University of Texas at Austin was made possible under a limited license grant from the author who has retained all copyrights in the works.en
dc.subject.lcshDielectricsen
dc.subject.lcshGate array circuitsen
dc.subject.lcshElectromotive forceen
dc.subject.lcshMetal oxide semiconductor field-effect transistorsen
dc.titleThe mechanism of the flatband voltage shift by capping a thin layer of Me₂O₃ (Me=Gd, Y and Dy) on SiO₂ and HfO₂-based dielectricsen
thesis.degree.departmentElectrical and Computer Engineeringen
thesis.degree.disciplineElectrical and Computer Engineeringen
thesis.degree.grantorThe University of Texas at Austinen
thesis.degree.levelDoctoralen
thesis.degree.nameDoctor of Philosophyen

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