ABSTRACT

In the field of microelectronics, the planar silicon metal-oxide-semiconductor field-effect transistor (MOSFET) is perhaps the most important invention. It started in 1928 when J. E. Lilienfeld proposed the concept of field-effect conductivity modulation and the MOSFET. William Shockley, John Bardeen, and Walter Brattain invented the transistor in 1947, and with the discovery of silicon dioxide (SiO2) passivation for the Si by Atalla in 1958, the Si MOSFET era started. Since then MOSFET performance has been improved at a dramatic rate via gate length scaling, and complementary metal-oxide-semiconductor (CMOS) is currently the dominant technology for integrated circuits. As the technology scales almost every 2 years, the transistor integration capacity doubles (Moore’s law), gate delay reduces by 30%, energy per logic operation reduces by 65%, and power consumption reduces by 50%. Table 1.1 shows CMOS technology outlook extrapolated from the current International Technology Roadmap for Semiconductors (ITRS) trends. However, conventional CMOS scaling has now approached the fundamental limits, which include leakage in channel and gate, diminished bulk effect, transport in silicon, and increased power dissipation. The huge costs of scaling CMOS devices according to Moore’s law have now left the silicon industry at a crossroad. As technology scales, the cost of a transistor goes down, but the cost of fabrication facilities, cost of mask set, and turnaround time increase for each generation. Lithographic challenges for future technology nodes have become a major concern. Implementation of extreme ultraviolet radiation (EUV) will help continue transistor size scaling. Although it will allow for increased device density, current scaling issues will be a major concern at smaller gate length devices. ITRS 2009 has projected scaling of the advanced MOSFETs covering the next 15 years through 2022. The evolution of the Si process technology after the 130 nm node is shown in Figure 1.1. Technology challenges for 10 nm CMOS and beyond will face process limitations such as patterning ultra-fine and random features, ultra-thin gate dielectric (∼3 Ǻ), and ultra-shallow junction (∼3 nm). In the following, we shall address the recent developments, which have been the subject of a major research drive for the last 10 years aimed at finding new avenues to enhance the performance of MOSFETs.