Hot electron currents in MOSFETs.

Silicon has become the material of choice for fabrication of high circuit density, low defect density and high speed integration devices. CMOS technology has been favoured as an attractive candidate to take advantage of the performance enhancements available through miniturisation. However, hot carrier effects in general, and hot electron currents in particular, are posing as the main obstacle to a new era of sub-micron architecture in semiconductor device technology. Electron transport in modern sub-micron device is often governed by mechanisms that were not relevant to long-channel devices. Many of the classical device models are based upon such convenient assumptions as "thermal equilibrium" and "uniform local electric field". With the downscaling of devices, hot electron currents are becoming increasingly inherent. These currents arise from the fact that electrical fields in small geometry devices can reach very high values and can vary rapidly in space. The large electric field can Impart significant kinetic energies to the carriers. In thermal equilibrium, all elementary excitations in a semiconductor (eg. Electrons, holes, phonons) can be characterised by a temperature that is the same as the lattice temperature. Under the influence of large electric fields, however, the distribution function of these elementally excitations deviate from those in thermal equilibrium. The term "Hot Carriers" is often used to describe these non-equilibrium situations. In this thesis hot electron currents, in particular their physical origins and dependence upon various operational and geometrical parameters, have been discussed and then quantified in a number of models based on the "Lucky Drift" theory of transport. Temperature is then used as a tool to differentiate between the underlying physical processes, and to determine if reliability problems related to hot electron effects would improve under cryogenic operation. It has been the prime objective of this work from the outset to concentrate on the study of N-channel devices. This is primarily due to the fact that N-channel MOSFET's are more prone to hot electron effects, and therefore, studies in the nature of this enhanced susceptibility could prove to be more fruitful

Simulation of hot carriers in semiconductor devices

Thesis (Ph. D.)--Massachusetts Institute of Technology, Dept. of Electrical Engineering and Computer Science, 1995.Includes bibliographical references (p. 109-113).by Khalid Rahmat.Ph.D

Simulation of hot carriers in semiconductor devices

Includes bibliographical references (p. 109-113).Supported by the U.S. Navy. N00174-93-C-0035Khalid Rahmat

Scaling the bulk-driven MOSFET into deca-nanometer bulk CMOS technologies

The International Technology Roadmap for Semiconductors predicts that the nominal power supply voltage, VDD, will fall to 0.7 V by the end of the bulk CMOS era. At that time, it is expected that the long-channel threshold voltage of a MOSFET, VT0, will rise to 35.5% of VDD in order to maintain acceptable off-state leakage characteristics in digital systems. Given the recent push for system-on-a-chip integration, this increasing trend in VT0/VDD poses a serious threat to the future of analog design because it causes traditional analog circuit topologies to experience progressively problematic signal swing limitations in each new process generation. To combat the process-scaling-induced signal swing limitations of analog circuitry, researchers have proposed the use of bulk-driven MOSFETs. By using the bulk terminal as an input rather than the gate, the bulk-driven MOSFET makes it possible to extend the applicability of any analog cell to extremely low power supply voltages because VT0 does not appear in the device\u27s input signal path. Since the viability of the bulk-driven technique was first investigated in a 2 um p-well process, there have been numerous reports of low-voltage analog designs incorporating bulk-driven MOSFETs in the literature - most of which appear in technologies with feature sizes larger than 0.18 um. However, as of yet, no effort has been undertaken to understand how sub-micron process scaling trends have influenced the performance of a bulk-driven MOSFET, let alone make the device more adaptable to the deca-nanometer technologies widely used in the analog realm today. Thus, to further the field\u27s understanding of the bulk-driven MOSFET, this dissertation aims to examine the implications of scaling the device into a standard 90 nm bulk CMOS process. This dissertation also describes how the major disadvantages of a bulk-driven MOSFET - i.e., its reduced intrinsic gain, its limited frequency response and its large layout area requirement - can be mitigated through modifications to the device\u27s vertical doping profile and well structure. To gauge the potency of the proposed process changes, an optimized n-type bulk-driven MOSFET has been designed in a standard 90 nm bulk CMOS process via the 2-D device simulator, ATLAS