Time-dependent gate oxide breakdown

About: Time-dependent gate oxide breakdown is a research topic. Over the lifetime, 5740 publications have been published within this topic receiving 95381 citations.

High-electron mobility transistor with zinc oxide

Abstract: A zinc oxide (ZnO) field effect transistor exhibits large input amplitude by using a gate insulating layer. A channel layer and the gate insulating layer are sequentially laminated on a substrate. A gate electrode is formed on the gate insulating layer. A source contact and a drain contact are disposed at the both sides of the gate contact and are electrically connected to the channel layer via openings. The channel layer is formed from n-type ZnO. The gate insulating layer is made from aluminum nitride/aluminum gallium nitride (AlN/AlGaN) or magnesium zinc oxide (MgZnO), which exhibits excellent insulation characteristics, thus increasing the Schottky barrier and achieving large input amplitude. If the FET is operated in the enhancement mode, it is operable in a manner similar to a silicon metal oxide semiconductor field effect transistor (Si-MOS-type FET), resulting in the formation of an inversion layer.

Vertical scaling of carbon nanotube field-effect transistors using top gate electrodes

Abstract: We have fabricated single-wall carbon nanotube field-effect transistors (CNFETs) in a conventional metal–oxide–semiconductor field-effect transistor (MOSFET) structure, with gate electrodes above the conduction channel separated from the channel by a thin dielectric These top gate devices exhibit excellent electrical characteristics, including steep subthreshold slope and high transconductance, at gate voltages close to 1 V—a significant improvement relative to previously reported CNFETs which used the substrate as a gate and a thicker gate dielectric Our measured device performance also compares very well to state-of-the-art silicon devices These results are observed for both p- and n-type devices, and they suggest that CNFETs may be competitive with Si MOSFETs for future nanoelectronic applications

MOSFET having a double gate

Abstract: A double gate MOSFET. The MOSFET includes a bottom gate electrode and a bottom gate dielectric disposed over the bottom gate electrode. A semiconductor body region is disposed over the bottom gate dielectric and the bottom gate electrode, and disposed between a source and a drain. A top gate electrode is disposed over the body. A top gate dielectric separates the top gate electrode and the body, the top gate electrode and the bottom gate electrode defining a channel within the body and interposed between the source and the drain. At least one of the bottom gate dielectric or the top gate dielectric is formed from a high-K material. A method of forming a double gate MOSFET is also disclosed where a semiconductor film used to form a body is recrystallized using a semiconductor substrate as a seed crystal.

New insights in the relation between electron trap generation and the statistical properties of oxide breakdown

Abstract: In this paper it is demonstrated in a wide stress field range that breakdown in thin oxide layers occurs as soon as a critical density of neutral electron traps in the oxide is reached. It is proven that this corresponds to a critical hole fluence, since a unique relationship between electron trap generation and hole fluence is found independent of stress field and oxide thickness. In this way literature models relating breakdown to hole fluence or to trap generation are linked. A new model for intrinsic breakdown, based on a percolation concept, is proposed. It is shown that this model can explain the experimentally observed statistical features of the breakdown distribution, such as the increasing spread of the Q/sub BD/-distribution for ultrathin oxides. An important consequence of this large spread is the strong area dependence of the Q/sub BD/ for ultrathin oxides.

High-K materials and metal gates for CMOS applications

Abstract: The scaling of complementary metal oxide semiconductor (CMOS) transistors has led to the silicon dioxide layer used as a gate dielectric becoming so thin that the gate leakage current becomes too large. This led to the replacement of SiO2 by a physically thicker layer of a higher dielectric constant or ‘high-K’ oxide such as hafnium oxide. Intensive research was carried out to develop these oxides into high quality electronic materials. In addition, the incorporation of Ge in the CMOS transistor structure has been employed to enable higher carrier mobility and performance. This review covers both scientific and technological issues related to the high-K gate stack – the choice of oxides, their deposition, their structural and metallurgical behaviour, atomic diffusion, interface structure, their electronic structure, band offsets, electronic defects, charge trapping and conduction mechanisms, reliability, mobility degradation and oxygen scavenging to achieve the thinnest oxide thicknesses. The high K oxides were implemented in conjunction with a replacement of polycrystalline Si gate electrodes with metal gates. The strong metallurgical interactions between the gate electrodes and the HfO2 which resulted an unstable gate threshold voltage resulted in the use of the lower temperature ‘gate last’ process flow, in addition to the standard ‘gate first’ approach. Work function control by metal gate electrodes and by oxide dipole layers is discussed. The problems associated with high K oxides on Ge channels are also discussed.