Learn the basic properties and designs of modern VLSI devices, as well as the factors affecting performance, with this thoroughly updated second edition. The first edition has been widely adopted as a standard textbook in microelectronics in many major US universities and worldwide. The internationally-renowned authors highlight the intricate interdependencies and subtle tradeoffs between various practically important device parameters, and also provide an in-depth discussion of device scaling and scaling limits of CMOS and bipolar devices. Equations and parameters provided are checked continuously against the reality of silicon data, making the book equally useful in practical transistor design and in the classroom. Every chapter has been updated to include the latest developments, such as MOSFET scale length theory, high-field transport model, and SiGe-base bipolar devices.

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Fundamentals of Modern VLSI Devices

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

In fabricating a thin film transistor, an active layer comprising a silicon semiconductor is formed on a substrate having an insulating surface Hydrogen is introduced into The active layer A thin film comprising SiO x N y is formed to cover the active layer and then a gate insulating film comprising a silicon oxide film formed on the thin film comprising SiO x N y  Also, a thin film comprising SiO x N y is formed under the active layer The active layer includes a metal element at a concentration of 1×10 15 to 1×10 19 cm −3 and hydrogen at a concentration of 2×10 19 to 5×10 21 cm −3 

Semiconductor device and method for forming the same

Silicon germanium (SiGe) has moved from being a research material to accounting for a small but significant percentage of manufactured semiconductor devices. This percentage is predicted to increase substantially as SiGe begins to be used in complementary metal oxide semiconductor (CMOS) technology in the future to substantially improve performance. It is the development of Si/SiGe heterostructures which has enabled band structure and strain engineering allowing Si/SiGe to be used in many different ways to improve conventional microelectronic device performance along with allowing new concepts to be explored. This paper presents a review of the material properties, growth techniques, band structure and the main electronic devices of the Si/SiGe heterostructure system. In particular, the important device technologies in mainstream microelectronics of the SiGe heterostructure bipolar transistor (HBT) and strained-Si CMOS will be reviewed before future device and optoelectronics concepts are explored.

https://iopscience.iop.org/article/10.1088/0268-1242/19/10/R02/pdf

Si/SiGe heterostructures: from material and physics to devices and circuits

A process is described for manufacturing an improved PMOS semiconductor transistor. Recesses are etched into a layer of epitaxial silicon. Source and drain films are deposited in the recesses. The source and drain films are made of an alloy of silicon and germanium. The alloy is epitaxially deposited on the layer of silicon. The alloy thus has a lattice having the same structure as the structure of the lattice of the layer of silicon. However, due to the inclusion of the germanium, the lattice of the alloy has a larger spacing than the spacing of the lattice of the layer of silicon. The larger spacing creates a stress in a channel of the transistor between the source and drain films. The stress increases IDSAT and IDLIN of the transistor. An NMOS transistor can be manufactured in a similar manner by including carbon instead of germanium, thereby creating a tensile stress.

Semiconductor transistor having a stressed channel

A structure of a semiconductor device and a method of manufacturing the same is provided wherein a leakage current can be reduced while improving a drain breakdown voltage of an Insulated-Gate transistor such as a MOSFET, MOSSIT and a MISFET, and a holding characteristic of a memory cell such as a DRAM using these transistors as switching transistors can be improved, and further a reliability of a gate oxide film in a transfer gate can be improved. More particularly, a narrow band gap semiconductor region such as Six Ge1-x, Six Sn1-x, PbS is formed in an interior of a source region or a drain region in the SOI.IG-device. By selecting location and/or mole fraction of the narrow band gap semiconductor region in a SOI film, or selecting a kind of impurity element to compensate the crystal lattice mismatching due to the narrow-bandgap semiconductor region, the generation of crystal defects can be suppressed. Further the structure that the influences of the crystal defects to the transistor or memory characteristics such as the leakage current can be suppressed, even if the crystal defects are generated, are also proposed.

Insulated-gate transistor having narrow-bandgap-source

Thinning effects on the device characteristics of silicon-on-insulator (SOI) MOSFETs are discussed. Two-dimensional/two-carrier device simulation revealed the following advantages. An n-channel MOSFET with 500-AA-SOI thickness exhibited a high-punchthrough resistance as well as an improved subthreshold swing down to a deep submicrometer region, even if the film was nearly intrinsic. A capacitance coupling model has been proposed to explain these subthreshold characteristics. The kink elimination effect, which was attributed to a significantly reduced hole density in the SOI film, was reproduced. The low-field channel mobility exhibited a significant increase, which was ascribed to a decrease in the vertical electric field. Moreover, the current-overshoot phenomenon associated with the switching operation was suppressed. Excess holes recombine with electrons quickly after the gate turn-on, bringing about a stabilized potential in the SOI substrate. Experiments were also carried out to verify the simulation. >

Two-dimensional simulation and measurement of high-performance MOSFETs made on a very thin SOI film

The drain breakdown phenomenon in ultra-thin-film (silicon-on-insulator) SOI MOSFETs has been studied. Two-dimensional simulation revealed that the thinning of the SOI film brings about an increase in the drain electric field due to the two-dimensional effect, causing a significant lowering in the drain breakdown voltage, as has been commonly seen in ultra-thin-film SOI MOSFETs. The simulation also showed that the lowered drain breakdown voltage recovered almost to its original value when the drain SOI thickness was restored, suggesting that the drain structure, rather than the source, plays a major role in determining the drain breakdown voltage. Experiments using an asymmetric device structure supported this hypothesis, showing that the breakdown voltage was mostly dependent on the drain structure, the initial potential barrier height at the source-SOI-body junction being only a minor factor. Transient simulation was also carried out to investigate the detailed breakdown process, showing that holes accumulate near the source-SOI-body junction at a high drain bias, eventually forward-biasing the junction. These results indicate that a careful drain design and/or proper choice of the SOI thickness as well as the supply voltage are quite important for realizing high performance of ultra-thin-film SOI MOSFETs. >

Analysis of the drain breakdown mechanism in ultra-thin-film SOI MOSFETs

The present invention provides a semiconductor device which includes a substrate having a projection-shaped semiconductor element region, a gate electrode formed through a gate insulating film on the upper face and side face of the element region, and a first conductivity type source region and drain region provided in a manner to form a channel region on the upper face of the element region across the gate electrode, and which has a high concentration impurity region containing a second conductivity type impurity at a concentration higher than that on the surface of the channel region in the central part of the projection-shaped semiconductor element region.

Semiconductor device having a projecting element region

In this paper, a novel lateral bipolar transistor on thin film silicon-on-insulator (SOI) is presented. With a small emitter size of 0.12/spl times/3.0 /spl mu/m/sup 2/, low base resistance of 270 /spl Omega/ due to a novel Co silicided base electrode and low base-collector parasitic capacitances of 1.4 fF due to SOI material, it achieves the highest f/sub max/ of 67 GHz among SOI bipolar transistors. Also, the low emitter-base capacitance of 1.5 fF and the low collector-substrate capacitance of 2.5 fF are realized. The transistor has a simple structure, which is fabricated with simplified processes without any new sophisticated technologies, excluding trench isolation and epitaxial base used in current bipolar transistors. This can lower the fabrication cost of transistors. We have demonstrated the possibility of lateral bipolar transistor on thin film SOI as next-generation device for RF analog applications.

Makoto Yoshimi

Papers

Insulated-gate transistor having narrow-bandgap-source

Two-dimensional simulation and measurement of high-performance MOSFETs made on a very thin SOI film

Analysis of the drain breakdown mechanism in ultra-thin-film SOI MOSFETs

Semiconductor device having a projecting element region

A novel lateral bipolar transistor with 67 GHz f/sub max/ on thin-film SOI for RF analog applications