This letter reports a charge collection experiment of alpha-particle-induced carriers in the cell arrays of the 1 Mb DRAM. It is indicated that this experiment is effective to estimate the soft error rate of VLSI memories with various kinds of structures.

A novel isolation structure which has a buried insulator between polysilicon electrodes (BIPS) has been developed. The BIPS isolation employs the refilling CVD-oxides in openings between polysilicon electrodes by photoresist etchback process. Device characteristics and parasitic effects of BIPS isolation have been compared with that of LOCOS isolation. Using BIPS isolation, we can almost suppress the narrow-channel effects and achieve the deep submicron isolation. No degradation on the subthreshold decay of devices with BIPS isolation can be obtained. The use of BIPS isolation technology yields a DRAM cell of small area. The successful fabrication of deep submicron devices with BIPS isolation clearly demonstrates that this technology has superior ability to overcome the LOCOS isolation.

The progress of LSI technologies makes it possible to fabricate 256 MDRAM. However, it depends on the cost effectiveness of device fabrication that LSI memory can continue to be the technology driver or not. It is indispensable to make the device, process, and equipment as simple as possible for next generation LSI. For example, wavefront technologies in lithography, high energy ion implantation, and simple DRAM cell with SOI structure or high dielectric constant capacitor, are under development to satisfy both device performance improvement and process simplicity.

A novel CMOS structure has been developed using Ti-salicide PSD transistor formed by a new self-aligned method. Both N-channel and P-channel PSD transistors exhibit excellent short-channel behaviors down to the sub-half-micrometer region with shallow S/D junctions formed by dopant diffusion from polysilicons. New salicide process has been developed for the PSD structure and can effectively reduce the sheet resistances of the S/D polysilicon and the polysilicon gate to as low as 45Ω/. As a result, the low resistive local interconnects can be successfully implemented by the Ti-salicide S/D polysilicon merged with contacts by self-alignment. More-over it is found that shallow Ti-salicide S/D junctions with the PSD structure can achieve approximately 12 orders of magnitude lower area leakage current than that of the conventional implanted S/D junctions by eliminating implanted damage and preventing penetration of silicide into junctions with the elevated structure of S/D polysilicon layer. Furthermore CMOS ring oscillators having PSD transistors with an effective channel length of 0.4 µm were fabricated using the salicided S/D polysilicon as a local interconnect between the N+ and the P+ regions, and successfully operated with a propagation delay time of 50 ps/stage at a supply voltage of 5 V.

Thin- and ultra-thin-film SOI MOSFET's are promising candidates to overcome the constraints for future miniaturized devices. This paper presents simulation results for a 0.1 µm gate length SOI MOSFET structure using a two-dimensional/two-carrier device simulator with a nonlocal model for the avalanche induced carrier generation. For the suppression of punchthrough effect in devices with a channel doping of 1 1016 cm-3 and 5 nm thick gate oxide it is found that the SOI layer thickness has to be reduced to at least 20 nm. The thickness of the buried oxide should not be smaller than 50 nm in order to avoid the degradation of thin SOI performance advantages. Investigating ways to suppress the degradation of the sub-threshold slope factor at these device dimensions it was found in contrast to the common expectation that the S-factor can be improved by increasing the body doping concentration. This phenomenon, which is a unique feature of thin-film depleted SOI MOSFET's, is explained by an analytical mode. At lower doping the area of the current flow is reduced by a decreasing effective channel thickness resulting in a slope factor degradation. Other approaches for S-factor improvement are the reduction of the channel edge capacitances by source/drain engineering or the decrease of SOI thickness or gate oxide thickness. For the latter approach a higher permittivity gate insulating material should be used in order to prevent tunnelling. The low breakdown voltage can be increased by utilizing an LDD structure to be suitable for a 1.5 V power supply. However, this is at the expense of reduced current drive. An alternative could be the supply voltage reduction to 1.0 V for single drain structure use. A dual-gated SOI MOSFET has an improved performance due to the parallel combination of two MOSFET's in this device. A slightly reduced breakdown voltage indicates a larger drain electric field present in this structure.

Hot-carrier characteristics in ultra-thin SOI MOSFET's (T-SOI MOSFET's) with gate-overlapped LDD have been investigated. The change in transistor static characteristics after hot carrier stress was mainly observed as positive threshold voltage (Vt) shifts due to trapped electrons, while in bulk-Si MOSFET's drain current degradation was dominant. The hot-carrier life time in T-SOI MOSFET's was comparable to that in bulk-Si devices at low drain voltage, but the life time dependence on drain voltage was different from that in bulk-Si MOSFET's, and the Vt degraded rapidly at the condition that parasitic bipolar breakdown began to occur. This implies that the drain supply voltage in T-SOI MOSFET's is determined directly by parasitic bipolar breakdown voltage unlike bulk-Si MOSFET's in which it is determined by hot-carrier reliability. The gate-overlapped LDD structure was compared with single drain structure and proved to provide better hot-carrier endurance by the improvement of the parasitic bipolar breakdown voltage. The hot-carrier reliability in the back channels of T-SOI MOSFET's was also investigated, and it was found that the back channel tends to be degraded more easily than front channel with large positive Vt shifts. These results suggest that the front Vt shifts in T-SOI devices are related with electron injection into the back surface of the T-SOI layer through charge coupling at the condition that the parasitic bipolar breakdown occurs.