New channel engineering for sub-100 nm MOS devices considering bothcarrier velocity overshoot and statistical performance fluctuations

We introduce a new channel engineering design for nano-region SOI and bulk MOSFETs taking into account both carrier velocity overshoot and statistical performance fluctuations. For types of both device, in the high gate drive region, the high field carrier velocity υ_e is not degraded at channel dopant density N_a lower than 1×10¹⁷ cm^-3, according to an experimental universal relationship between υ_e and the low field mobility. On the other hand, there is a most suitable N_a condition for suppression of statistical threshold voltage fluctuations. This most suitable N_a is slightly higher for SOI devices than that for bulk MOSFETs, but it is lower than 1×10 ¹⁷ cm^-3 in both cases. Therefore, this most suitable N_a condition is consistent with the above N_a condition for carrier velocity. Consequently, new N_a conditions for nano region devices are introduced in this study. N_a should be designed to be of the order of 1×10¹⁶ cm^-3 rather than rising by the usual scaling rule, but it is necessary to suppress the short channel effects of SOI and bulk MOSFETs by scaling down the SOI thickness, and to use source/drain junction depth scaling or surface low impurity structures in bulk MOSFETs, respectively     

The characteristics of CMOS devices in oxygen-implantedsilicon-on-insulator structures

The characteristics of CMOS devices fabricated in oxygen-implanted silicon-on-insulator (SOI) substrates with different oxygen doses are studied. The results show that transistor junction leakage currents are improved by orders of magnitude when the oxygen dose is decreased from 2.25×10¹⁸ cm^-2 to 1.4×10¹⁸ cm^-2 . The floating-body effect, i.e. transistor turn-on at lower gate voltage with dramatic improvement in subthreshold slope when the drain voltage is increased, is enhanced by the reduction in leakage current and hence the oxygen dose. In SOI substrates implanted with 1.4×10¹⁷ cm^-2 oxygen dose and annealed at 1150°C, back-channel mobilities are decreased by several orders of magnitude compared to the mobilities in the precipitate-free silicon film. These device characteristics are correlated with the microstructure at the silicon-buried-oxide interface, which is controlled by oxygen implantation and post-oxygen-implantation anneal     

High-mobility ultrathin strained Ge MOSFETs on bulk and SOI with low band-to-band tunneling leakage: experiments

For the first time, the tradeoffs between higher mobility (smaller bandgap) channel and lower band-to-band tunneling (BTBT) leakage have been investigated. In particular, through detailed experiments and simulations, the transport and leakage in ultrathin (UT) strained germanium (Ge) MOSFETs on bulk and silicon-on-insulator (SOI) have been examined. In the case of strained Ge MOSFETs on bulk Si, the resulting optimal structure obtained was a UT low-defect 2-nm fully strained Ge epi channel on relaxed Si, with a 4-nm Si cap layer. The fabricated device shows very high mobility enhancements >3.5/spl times/ over bulk Si devices, 2/spl times/ mobility enhancement and >10/spl times/ BTBT reduction over 4-nm strained Ge, and surface channel 50% strained SiGe devices. Strained SiGe MOSFETs having UT (T/sub Ge/<3 nm) very high Ge fraction (/spl sim/ 80%) channel and Si cap (T/sub Si cap/<3 nm) have also been successfully fabricated on thin relaxed SOI substrates (T/sub SOI/=9 nm). The tradeoffs in obtaining a high-mobility (smaller bandgap) channel with low tunneling leakage on UT-SOI have been investigated in detail. The fabricated device shows very high mobility enhancements of >4/spl times/ over bulk Si devices, >2.5/spl times/ over strained silicon directly on insulator (SSDOI; strained to 20% relaxed SiGe) devices, and >1.5/spl times/ over 60% strained SiGe (on relaxed bulk Si) devices.     

Confined lateral selective epitaxial growth of silicon for devicefabrication

An epitaxy technique, confined lateral selective epitaxial growth (CLSEG), which produces wide, thin slabs of single-crystal silicon over insulator, using only conventional processing, is discussed. As-grown films of CLSEG 0.9 μm thick, 8.0 μm wide, and 500 μm long were produced at 1000°C at reduced pressure. Junction diodes fabricated in CLSEG material show ideality factors of 1.05 with reverse leakage currents comparable to those of diodes built in SEG homoepitaxial material. Metal-gate p-channel MOSFETs in CLSEG with channel dopings of 2×10¹⁶ cm^-3 exhibit average mobilities of 283 cm²/V-s and subthreshold slopes of 223 mV/decade     

Novel SOI p-channel MOSFETs with higher strain in si channel usingdouble SiGe heterostructures

We have studied p-channel advanced SOI MOSFETs using double SiGe heterostructures fabricated by the combination of SIMOX and high-quality strained-Si/SiGe regrowth technologies, in order to introduce higher strain in Si channel. It was revealed that this double SiGe structure of second Si_0.82Ge_0.18Si_0.93Ge_0.07 allows the second SiGe layer to relax by about 70%, because of the elastic energy balance between the second and the first-SiGe layers. As a result, the strain of Si layer on this double SiGe structure becomes higher than that of the single SiGe structure. Strained SOI p-MOSFETs using the double layer SiGe structure exhibited higher hole mobility than that of strained-SOI MOSFETs with single Si_0.9Ge_0.1 structure. The hole mobility enhancement of 30% and 45% was achieved in the strained-SOI MOSFETs with double SiGe structures, compared to that of the universal curve and the control-SOI MOSFETs, respectively     

A CV technique for measuring thin SOI film thickness

A technique is developed to measure silicon-on-insulator (SOI) silicon device film thickness using a MOSFET. The method is based on CV measurements between gate and source/drain at two different back-gate voltages. The SOI devices used in this study were n⁺ polysilicon gate n-channel MOSFETs fabricated with modified submicrometer CMOS technology on SIMOX (separation by implanted oxygen) wafers. The SIMOX wafers were implanted with a high dose of oxygen ions (10¹⁸ cm^-2) at 200 keV and subsequently annealed at 1230°C. The NMOS threshold boron implant dose is 2×10¹² cm^-2. This method is simple, nondestructive, and no special test structure is needed. Using this technique, SOI film thickness mapping was made on a finished wafer and a thickness variation of ±150 Å was found     

Back-gated buried oxide MOSFETs in a high-voltage bipolartechnology for bonded oxide/SOI interface characterization

A novel back-gated P-MOSFET structure is fabricated in a high-voltage complementary bipolar technology using BESOI (bonded etch back SOI) substrates. The P+ buried layer regions, used for the PNP BJT are used as the source and drain regions, the N- epi as the channel region, the silicon handle wafer as the gate, and the BOX (buried oxide) as the gate oxide. The P-MOSFET was used to characterize the interface between the BOX and the SOI. The devices exhibit high sub-threshold slope which is attributed to a high interface state density of about 2×10¹²/cm² at the bonding interface. Bias-temperature stress measurements show an effective mobile charge density of 4×10¹⁰/cm² in the buried oxide     

Fabrication of SOS MOSFETs using two-step doping with excimer laser

Using two-step doping with excimer laser, p-channel MOSFETs were fabricated in thin silicon films on sapphire (SOS). Source and drain p ⁺ layers were formed using two-step doping with only one melting pulse of excimer laser. Devices were processed at room temperature except for the LPCVD gate oxide deposition at 450°C. High-quality thin film transistors (TFTs) were fabricated with on/off current ratio of 7 and a field effect hole mobility of 145 cm²/V s     

Hybrid Integration of Ultrathin-Body Partially Insulated MOSFETs and a Bulk MOSFET for Better IC Performance: A Multiple-$V_{rm TH}$ Technology Using Partial SOI Structure

The hybrid integration of ultrathin-body partially insulated MOSFETs (UTB PiFETs) and a bulk MOSFET was investigated. With a partial silicon-on-insulator (SOI) process using a SiGe sacrificial layer, UTB PiFETs with thin buried insulation layers were realized on the same bulk Si wafer with a bulk MOSFET. A partially insulating oxide (PiOX)-under-channel PiFET is suitable from the viewpoint of high-speed operation due to its SOI-like characteristics. On the other hand, a PUSD PiFET is useful from the viewpoint of low stand-by power operation due to its low junction leakage current. Through hybrid integration, not only multiple V_TH's can be obtained but also the technical difficulties of bulk MOSFETs can be alleviated. Thus, hybrid integration is a very useful process technique to implement integrated-circuit products with optimized power and performance management.     

Electrical characteristics of 4.5 kV implanted anode 4H-SiC p-i-njunction rectifiers

4500 V 4H-SiC p-i-n junction rectifiers with low on-state voltage drop (3.3-4.2 V), low reverse leakage current (3×10^-6 A/cm²), and fast switching (30-70 ns) have been fabricated and characterized. Forward current-voltage measurements indicate a minimum ideality factor of 1.2 which confirms a recombination process involving multiple energy levels. Reverse leakage current exhibits a square root dependence on voltage below the punchthrough voltage where leakage currents of less than 3×10^-6 A/cm² are measured. Reverse recovery measurements are presented which indicate the presence of recombination at the junction perimeter where a surface recombination velocity of 2-8×10⁵ cm/s is found. These measurements also indicate drift layer bulk carrier lifetimes ranging from 74 ns at room temperature to 580 ns at 250°C     

Monte Carlo simulation of p- and n-channel GOI MOSFETs by solving the quantum Boltzmann equation

The scaling characteristics of both n- and p-channel Ge-on-insulator (GOI) as well as silicon-on-insulator (SOI) MOSFETs with channel length ranging from 20-130 nm are studied by a two-dimensional self-consistent fullband Monte Carlo device simulator. The transistors' intrinsic performance and subthreshold characteristics are investigated for various channel lengths and Ge layer thicknesses. Our results indicate that both n- and p-channel GOI MOSFETs can be scaled down to the nanoregion, due to the nonstationary transport, especially for the p-channel device. More than 10% performance improvement for nMOS and about 20% for pMOS can be achieved in GOI even when channel length is scaled down to 20 nm, as compared to SOI devices. However, the GOI devices suffer from more severe short channel effect and have larger p-n junction leakage current as compared to SOI counterpart. For high-performance CMOS applications, GOI devices are feasible if the junction leakage can be reduced by optimizing the device structure.     

An 1800 V triple implanted vertical 6H-SiC MOSFET

6H silicon carbide vertical power MOSFETs with a blocking voltage of 1800 V have been fabricated. Applying a novel processing scheme, n ⁺ source regions, p-base regions and p-wells have been fabricated by three different ion implantation steps. Our SiC triple ion implanted MOSFETs have a lateral channel and a planar polysilicon gate electrode. The 1800 V blocking voltage of the devices is due to the avalanche breakdown of the reverse diode. The reverse current density is well below 200 μA/cm² for drain source voltages up to 90% of the breakdown voltage. The MOSFETs are normally off showing a threshold voltage of 2.7 V. The active area of 0.48 mm² delivers a forward drain current of 0.3 A at Y_GS=10 V and V _DS=8 V. The specific on resistance was determined to 82 mΩdcm² at 50 mV drain source voltage and at V_GS =10 V which corresponds to an uppermost acceptable oxide field strength of about 2.7 MV/cm. This specific on resistance is an order of magnitude lower than silicon DMOSFET's of the same blocking capability could offer     

NMOS device characteristics in electron-beam-recrystallized SOI

Characteristics of n-channel MOSFETs fabricated in cold-cathode electron-beam-recrystallized silicon-on-oxide layers have been examined. Assorted crystallographic defects exist in the recrystallized silicon layer, ranging from highly branched subgrain boundaries to widely spaced parallel subgrains and rows of threading dislocations. Some of these MOSFET transistors have characteristics approaching those fabricated in bulk silicon including ≈828 cm²/V-s electron surface mobilities and 130 mV/decade inverse subthreshold slopes. However, many of the devices tested exhibited leakage currents up to 10^-6 A/μm, resulting in high inverse subthreshold slopes and reduced threshold voltages. Some effects of crystal imperfections on device behavior are discussed     

Unpinned GaAs MOS capacitors and transistors

Metal-oxide-semiconductor (MOS) capacitors and field-effect transistors (MOSFETs) in the GaAs semiconductor system using an unpinned interface are described. The structures utilize plasma-enhanced chemical-vapor deposition (PECVD) for the silicon-dioxide insulator on GaAs that has been terminated with a few monolayers of silicon during growth by molecular beam epitaxy. Interface densities in the structures have been reduced to ~10¹² cm^-2·eV^-1 . High-frequency characteristics indicate strong inversion of both p-type and n-type GaAs. The excellent insulating quality of the oxide has allowed demonstration of quasi-static characteristics. MOSFETs operating in depletion mode with a transconductance of 60 mS/mm at 8.0-μm gate lengths have been fabricated     

Optimization of oxygen-implanted silicon substrates for CMOS devices by electrical characterization

The use of oxygen-implanted silicon substrates for CMOS SOI device technology has great potential for use in VLSI and radiation-hardened circuits. The electrical characterization of such substrates is described by reference to CMOS devices fabricated directly into them; no epitaxial silicon was grown. Electrical parameters were related to the oxygen-implantation conditions of dose and temperature. Thermally generated oxygen donors in the top silicon layer were identified as being responsible for threshold voltage shifts and resistivity changes that altered transistor characteristics. Suitable boron implants enabled electrical parameter control to be maintained. Full island-to-substrate electrical isolation was only achieved for oxygen doses greater than 1.6 × 10¹⁸cm^-2, a larger dose from that required to create stoichiometric SiO2. Channel mobilities and NMOS back-channel leakage currents were found to be dependent on oxygen implant temperature; as a result a favorable implant window of 460-510 °C was established to fabricate ring oscillators twice as fast as bulk silicon counterparts for the same power dissipation.     

Electron velocity overshoot at room and liquid nitrogentemperatures in silicon inversion layers

Effective electron velocities in silicon MOSFETs exceeding the bulk saturation values of 10⁷ cm/s at room temperature and 1.3×10⁷ cm/s at liquid-nitrogen temperature are inferred. This conclusion suggests that electron velocity overshoot occurs over a large portion of the device channel length. To infer this phenomenon, submicrometer-channel-length Si MOSFETs with lightly doped inversion layers were fabricated. These devices have low field mobility of 450 cm²/V-s and showed only slight short-channel effects. Effective carrier velocities are calculated from the saturated transconductance g_m at V_DS=1.5 V after correction for parasitic resistances of source and drain     

Vertical n-p-n bipolar transistors fabricated on buried oxide SOI

Vertical n-p-n bipolar transistors have been fabricated in silicon-on-insulator (SOI) films prepared by buried oxide implantation. Electrical device characteristics are shown to be comparable to those obtained on devices fabricated in bulk silicon, indicating no significant degradation owing to the buried oxide layer. Dielectric isolation in excess of 10¹¹Ω.cm and µ 3 × 10⁶V/cm is measured.     

4H-SiC MOSFETs utilizing the H2 surface cleaningtechnique

The H₂ cleaning technique was examined as the precleaning of the gate oxidation for 4H-SiC MOSFETs. The device had a channel width and length of 150 and 100 μm, fabricated on the p-type epitaxial layer of 3×10¹⁶ cm^-3. The gate oxidation was performed after the conventional RCA cleaning, and H₂ annealing at 1000°C. The obtained channel mobility depends on the pre-cleaning process strongly, and was achieved 20 cm²/N s in the H₂ annealed sample. The effective interface-state density was also measured by the MOS capacitors fabricated on the same chips, resulting 1.8×10¹² cm^-2 from the photo-induced C-V method     

Gate and drain currents in off-state buried-type p-channel LDDMOSFETs

The buried-type p-channel LDD MOSFETs biased at high positive gate voltage exhibit novel characteristics: (1) the ratio of the drain to gate currents is about 1×10^-3 to 5×10^-3; and (2) the gate and drain currents both are functions of only the gate voltage minus the n-well bias. Such characteristics are addressed based on the formation of the surface n ⁺ inversion layer due to the punchthrough of the buried channel to the underlying shallow p-n junction. The measured gate current is due to the Fowler-Nordheim tunneling of electrons from this inversion layer surface and the holes generated within the high-field oxide constitute the drain current. The n⁺ inversion layer surface potential is found to be equal to the n-well bias plus 0.55 V. As a result, both the oxide field and the gate and drain currents are independent of drain voltage     

High performance poly-Si TFTs fabricated using pulsed laserannealing and remote plasma CVD with low temperature processing

Key technologies for fabricating polycrystalline silicon thin film transistors (poly-Si TFTs) at a low temperature are discussed. Hydrogenated amorphous silicon films were crystallized by irradiation of a 30 ns-pulsed XeCl excimer laser. Crystalline grains were smaller than 100 nm. The density of localized trap states in poly-Si films was reduced to 4×10¹⁶ cm^-3 by plasma hydrogenation only for 30 seconds. Remote plasma chemical vapor deposition (CVD) using mesh electrodes realized a good interface of SiO ₂/Si with the interface trap density of 2.0×10¹⁰ cm^-2 eV^-1 at 270°C. Poly-Si TFTs were fabricated at 270°C using laser crystallization, plasma hydrogenation and remote plasma CVD. The carrier mobility was 640 cm²/Vs for n-channel TFTs and 400 cm²/Vs for p-channel TFTs. The threshold voltage was 0.8 V for n-channel TFTs and -1.5 V for p-channel TFTs. The leakage current of n-channel poly-Si TFTs was reduced from 2×10^-10 A/μm to 3×10^-13 A/μm at the gate voltage of -5 V using an offset gate electrode with an offset length of 1 μm