High leakage current in deep-submicrometer regimes is becoming a significant contributor to power dissipation of CMOS circuits as threshold voltage, channel length, and gate oxide thickness are reduced. Consequently, the identification and modeling of different leakage components is very important for estimation and reduction of leakage power, especially for low-power applications. This paper reviews various transistor intrinsic leakage mechanisms, including weak inversion, drain-induced barrier lowering, gate-induced drain leakage, and gate oxide tunneling. Channel engineering techniques including retrograde well and halo doping are explained as means to manage short-channel effects for continuous scaling of CMOS devices. Finally, the paper explores different circuit techniques to reduce the leakage power consumption.

Leakage current mechanisms and leakage reduction techniques in deep-submicrometer CMOS circuits

The scaling of complementary metal oxide semiconductor transistors has led to the silicon dioxide layer, used as a gate dielectric, being so thin (14?nm) that its leakage current is too large It is necessary to replace the SiO2 with a physically thicker layer of oxides of higher dielectric constant (?) or 'high K' gate oxides such as hafnium oxide and hafnium silicate These oxides had not been extensively studied like SiO2, and they were found to have inferior properties compared with SiO2, such as a tendency to crystallize and a high density of electronic defects Intensive research was needed to develop these oxides as high quality electronic materials This review covers both scientific and technological issues?the choice of oxides, their deposition, their structural and metallurgical behaviour, atomic diffusion, interface structure and reactions, their electronic structure, bonding, band offsets, electronic defects, charge trapping and conduction mechanisms, mobility degradation and flat band voltage shifts The oxygen vacancy is the dominant electron trap It is turning out that the oxides must be implemented in conjunction with metal gate electrodes, the development of which is further behind Issues about work function control in metal gate electrodes are discussed

https://iopscience.iop.org/article/10.1088/0034-4885/69/2/R02/pdf

High dielectric constant gate oxides for metal oxide Si transistors

An object is to provide a semiconductor device of which a manufacturing process is not complicated and by which cost can be suppressed, by forming a thin film transistor using an oxide semiconductor film typified by zinc oxide, and a manufacturing method thereof. For the semiconductor device, a gate electrode is formed over a substrate; a gate insulating film is formed covering the gate electrode; an oxide semiconductor film is formed over the gate insulating film; and a first conductive film and a second conductive film are formed over the oxide semiconductor film. The oxide semiconductor film has at least a crystallized region in a channel region.

Semiconductor device, and manufacturing method thereof

The scaling of complementary metal oxide semiconductor (CMOS) transistors has led to the silicon dioxide layer used as a gate dielectric becoming so thin (1.4 nm) that its leakage current is too large. It is necessary to replace the SiO2 with a physically thicker layer of oxides of higher dielectric constant (κ) or 'high K' gate oxides such as hafnium oxide and hafnium silicate. Little was known about such oxides, and it was soon found that in many respects they have inferior electronic properties to SiO2 ,s uch as a tendency to crystallise and a high concentration of electronic defects. Intensive research is underway to develop these oxides into new high quality electronic materials. This review covers the choice of oxides, their structural and metallurgical behaviour, atomic diffusion, their deposition, interface structure and reactions, their electronic structure, bonding, band offsets, mobility degradation, flat band voltage shifts and electronic defects. The use of high K oxides in capacitors of dynamic random access memories is also covered.

/pdf/high-dielectric-constant-oxides-cotu2e70vd.pdf

High dielectric constant oxides

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.

/pdf/high-k-materials-and-metal-gates-for-cmos-applications-4hs77i3c4a.pdf

High-K materials and metal gates for CMOS applications

We report here that Fermi pinning at the polysilicon/metal-oxide interface causes high threshold voltages in MOSFET devices. In Part I, we investigated the different gatestack regions and determined that the polysilicon/metal oxide interface plays a key role on the threshold voltages. Now in Part II, the effects of the interfacial bonding are examined by experiments with submonolayer atomic-layer deposition (ALD) metal oxides and atomistic simulation. Results indicate that pinning occurs due to the interfacial Si-Hf and Si-O-Al bonds for HfO/sub 2/ and Al/sub 2/O/sub 3/, respectively. Oxygen vacancies at polysilicon/HfO/sub 2/ interfaces also lead to Fermi pinning. This fundamental characteristic affects the observed polysilicon depletion.

Fermi-level pinning at the polysilicon/metal-oxide interface-Part II

Method for forming a semiconductor device having an capacitor, where the capacitor is in-laid in a cavity formed in the semiconductor substrate and part of a high density memory. One embodiment first forms a bottom electrode in the cavity and then fills the cavity with a sacrificial layer to allow chemical mechanical polishing (CMP) of at least one of the capacitor electrodes. After removing portions of the bottom electrode and portions of the sacrificial layer, a dielectric layer is formed. A top electrode is then formed over the dielectric layer. The dielectric layer so formed isolates the bottom electrode from the top electrode preventing shorting and leakage currents. In one embodiment, a single top electrode layer is formed for multiple bottom electrodes, reducing the complexity of the memory circuit.

Method for forming a semiconductor device

We report for the first time on a novel dual-metal gate CMOS integration on HfO/sub 2/ gate dielectric using TiN (PMOS) and TaSiN (NMOS) gate electrodes. Compared to a single metal integration, the dual-metal integration does not degrade gate leakage, mobility and charge trapping behavior. Promising preliminary TDDB data were obtained from dual-metal gate MOSFETs, while still delivering much improved gate leakage (10/sup 4/ - 10/sup 5/ X better than SiO/sub 2/).

Dual-metal gate CMOS with HfO 2 gate dielectric

A transistor device (19) utilizes a high K dielectric (24) between a gate electrode (16) and a substrate (12). The high K dielectric (24) is etched under the gate electrode (16) so that there is an area between the gate electrode (16) and the substrate (12) that is void of high K dielectric (24). The source/drains extensions (28 and 30) are minimized to extend substantially in alignment with the edge of gate dielectric (24) to reduce overlap with the gate dielectric (24). This results in reduced capacitance between the gate and the source/drain extensions. The void areas (20 and 22) between the gate and the substrate (12) may remain void or may be filled with a low K dielectric, or at least a dielectric that is not high K.

Transistor having a high K dielectric and short gate length and method therefor

In accordance with one embodiment of the present invention, a method is disclosed for forming a semiconductor device having an isolation region ( 601 ). A dielectric layer ( 108 ) is deposited and etched to form isolation regions ( 102, 605 ) having top portions that are narrower than their bottom portions, thereby a tapered isolation region is formed. Active regions ( 601, 603 ) are formed using an epitaxial process in the regions between the isolation regions. The resulting active regions ( 601, 603 ) have a greater amount of surface area near a top portion, than near a bottom portion. Transistors ( 721, 723 ) having opposite polarities are formed within the active areas.

William J. Taylor

Papers

Fermi-level pinning at the polysilicon/metal-oxide interface-Part II

Method for forming a semiconductor device

Dual-metal gate CMOS with HfO 2 gate dielectric

Transistor having a high K dielectric and short gate length and method therefor

Method for forming a semiconductor device with an opening in a dielectric layer