Evidence suggests that MOSFET degradation is due to interface-states generation by electrons having 3.7 eV and higher energies. This critical energy and the observed time dependence is explained with physical model involving the breaking of the ≡ Si s H bonds. The device lifetime τ is proportional to I_{sub}^{-2.9}I_{d}^{1.9}\Delta V_{t}^{1.5} . If I sub is large because of small L or large V d , etc., τ will be small. I sub (and possibly light emission) is thus a powerful predictor of τ. The proportionality constant has been found to vary by a factor of 100 for different technologies, offering hope for substantially better reliability through future improvements in dielectric /interface technologies. A simple physical model can relate the channel field E m to all the device parameters and bias voltages. Its use in interpreting and guiding hot-electron scaling are described. LDD structures can reduce E m and I sub and, when properly designed, reduce device degradation.

Hot-electron-induced MOSFET degradation&#8212;Model, monitor, and improvement

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

The phase-shifting mask consists of a normal transmission mask that has been coated with a transparent layer patterned to ensure that the optical phases of nearest apertures are opposite. Destructive interference between waves from adjacent apertures cancels some diffraction effects and increases the spatial resolution with which such patterns can be projected. A simple theory predicts a near doubling of resolution for illumination with partial incoherence σ < 0.3, and substantial improvements in resolution for σ < 0.7. Initial results obtained with a phase-shifting mask patterned with typical device structures by electron-beam lithography and exposed using a Mann 4800 10× tool reveals a 40-percent increase in usuable resolution with some structures printed at a resolution of 1000 lines/mm. Phase-shifting mask structures can be used to facilitate proximity printing with larger gaps between mask and wafer. Theory indicates that the increase in resolution is accompanied by a minimal decrease in depth of focus. Thus the phase-shifting mask may be the most desirable device for enhancing optical lithography resolution in the VLSI/VHSIC era.

Improving resolution in photolithography with a phase-shifting mask

Various embodiments for improved power devices as well as their methods of manufacture, packaging and circuitry incorporating the same for use in a wide variety of power electronic applications are disclosed. One aspect of the invention combines a number of charge balancing techniques and other techniques for reducing parasitic capacitance to arrive at different embodiments for power devices with improved voltage performance, higher switching speed, and lower on-resistance. Another aspect of the invention provides improved termination structures for low, medium and high voltage devices. Improved methods of fabrication for power devices are provided according to other aspects of the invention. Improvements to specific processing steps, such as formation of trenches, formation of dielectric layers inside trenches, formation of mesa structures and processes for reducing substrate thickness, among others, are presented. According to another aspect of the invention, charge balanced power devices incorporate temperature and current sensing elements such as diodes on the same die. Other aspects of the invention improve equivalent series resistance (ESR) for power devices, incorporate additional circuitry on the same chip as the power device and provide improvements to the packaging of charge balanced power devices.

Power semiconductor devices and methods of manufacture

Evidence suggests that MOSFET degradation is due to interface-states generation by electrons having 3.7 eV and higher energies. This critical energy and the observed time dependence is explained with a physical model involving the breaking of the = Si/sub s/H bonds. The device lifetime /spl tau/ is proportional to...

Hot-Electron-Induced MOSFET Degradation - Model, Monitor, and Improvement

Building on nearly two decades of reported results for MOSFET's fabricated in small-grain polycrystalline silicon, a design methodology is developed that yields devices which have low threshold voltage, high drive current, low leakage current, tight parameteric control, and reduced topology, while requiring no nonstandard materials, processes, and tools. Design criteria and device performance are discussed, grain boundary characterization techniques are described, technological issues pertinent to VLSI implementation are investigated, and long-term device reliability is studied. The potential applications of the polysilicon MOSFET's in high-density dRAM and sRAM are explored. The successful implementation of an experimental stacked CMOS 64K static RAM proves the utility of these devices for three-dimensional integration in a VLSI environment.

Characteristics and three-dimensional integration of MOSFET's in small-grain LPCVD polycrystalline Silicon

DRAM cells and arrays of cells on a semiconductor substrate, together with methods of fabrication, are disclosed wherein the cells are formed in pairs or quartets by excavating a trench or two trenches through the cell elements to split an original cell into two or four cells during the fabrication. The cells include vertical field effect transistors and capacitors along the trench sidewalls with word lines and bit lines crossing over the cells.

Vertical DRAM cell and method

Circuit requirements of scaled devices based on noise margin, parameter variation, parasitic resistance and drift velocity saturation lead to non-constant field scaling, which predict a maximum in performance as devices are scaled. This maximum occurs at a smaller length for p-channel than for n-channel for a given scaling rule, and causes the performance of the two to approach each other at L<0.3µm. The p-channel devices under these conditions are shown to be 100x less effected by hot carriers induced reliability problems than n-channel devices.

The impact of scaling laws on the choice of n-channel or p-channel for MOS VLSI

A 1T DRAM cell with both the transistor and the capacitor fabricated on the sidewalls of a deep trench is described. Trench Transistor Cell (TTC) fabrication and characterization are discussed.

http://ieeexplore.ieee.org/iel5/9951/31947/01485625.pdf

A trench transistor cross-point DRAM cell

A dRAM cell and array of cells, together with a method of fabrication, are disclosed wherein the cell includes one field effect transistor and one storage capacitor with the capacitor formed in a trench in a substrate and the transistor channel formed by epitaxial growth on the substrate. The transistor source and drain are insulated from the substrate, and the transistor may be adjacent the trench or on the upper portion of the trench sidewalls. Signal charge is stored on the capacitor plate insulated from the substrate.

Pallab K. Chatterjee

Papers

Characteristics and three-dimensional integration of MOSFET's in small-grain LPCVD polycrystalline Silicon

Vertical DRAM cell and method

The impact of scaling laws on the choice of n-channel or p-channel for MOS VLSI

A trench transistor cross-point DRAM cell

DRAM Cell with trench capacitor and vertical channel in substrate