Design and fabrication of RESURF MOSFETs on 4H-SiC(0001), (112~0), and 6H-SiC(0001)

Design and fabrication of lateral SiC reduced surface field (RESURF) MOSFETs have been investigated. The doping concentration (dose) of the RESURF and lightly doped drain regions has been optimized to reduce the electric field crowding at the drain edge or in the gate oxide by using device simulation. The optimum oxidation condition depends on the polytype: N/sub 2/O oxidation at 1300/spl deg/C seems to be suitable for 4H-SiC, and dry O/sub 2/ oxidation at 1250/spl deg/C for 6H-SiC. The average inversion-channel mobility is 22, 78, and 68 cm/sup 2//Vs for 4H-SiC(0001), (112~0), and 6H-SiC(0001) MOSFETs, respectively. RESURF MOSFETs have been fabricated on 10-/spl mu/m-thick p-type 4H-SiC(0001), (112~0), and 6H-SiC(0001) epilayers with an acceptor concentration of 1/spl times/10/sup 16/ cm/sup -3/. A 6H-SiC(0001) RESURF MOSFET with a 3-/spl mu/m channel length exhibits a high breakdown voltage of 1620 V and an on-resistance of 234 m/spl Omega//spl middot/cm/sup 2/. A 4H-SiC(112~0) RESURF MOSFET shows the characteristics of 1230 V-138 m/spl Omega//spl middot/cm/sup 2/.     

1330 V, 67 m/spl Omega//spl middot/cm/sup 2/ 4H-SiC(0001) RESURF MOSFET

Design and fabrication of 4H-SiC(0001) lateral MOSFETs with a two-zone reduced surface field structure have been investigated. The dose dependencies of experimental breakdown voltage show good agreement with simulation. Through the optimization of implant dose, high-temperature (1700/spl deg/C) annealing after ion implantation, and reduction of channel length, a breakdown voltage of 1330 V and a low on-resistance of 67 m/spl Omega//spl middot/cm/sup 2/ have been obtained. The figure-of-merit (V/sub B//sup 2//R/sub on/) of the present device reaches 26 MW/cm/sup 2/, being the best performance among lateral MOSFETs reported. The temperature dependence of static characteristics is also presented.     

Design criteria of high-Voltage lateral RESURF JFETs on 4H-SiC

Integrated power electronics on SiC have great potential in future power electronics applications. In this paper, a novel vertical channel lateral junction field-effect transistor structure with reduced surface electric field effect is proposed for the first time on 4 H-SiC to address existing challenges in lateral power devices on SiC. Based on an experimentally proven channel design, the detailed design procedure of such a device has been investigated. Design criteria to optimize device forward blocking as well as conduction characteristics are studied. Parameter tolerance and design windows are discussed considering practical issues in device fabrication. Designs that will lead to an optimized tradeoff between device breakdown voltage and specific on-resistance are shown. With an 8-/spl mu/m-long drift region, a 1535-V breakdown voltage and 3.24 m/spl Omega//spl middot/cm/sup 2/ specific on-resistance can be achieved. This represents a figure-of-merit of 737 MW/cm/sup 2/, about 100 times higher than that of the best normally off lateral power devices reported in the literature. The proposed device can be an attractive candidate for power integrated circuit on SiC.     

Improved high-voltage lateral RESURF MOSFETs in 4H-SiC

High-voltage lateral RESURF metal oxide semiconductor field effect transistors (MOSFETs) in 4H-SiC have been experimentally demonstrated, that block 900 V with a specific on-resistance of 0.5 Ω-cm² . The RESURF dose in 4H-SiC to maximize the avalanche breakdown voltage is almost an order of magnitude higher than that of silicon; however this high RESURF dose leads to oxide breakdown and reliability concerns in thin (100-200 nm) gate oxide devices due to high electric field (>3-4 MV/cm) in the oxide. Lighter RESURF doses and/or thicker gate oxides are required in SiC lateral MOSFETs to achieve highest breakdown voltage capability     

High-voltage normally off GaN MOSFETs on sapphire substrates

Gallium nitride self-aligned MOSFETs were fabricated using low-pressure chemical vapor-deposited silicon dioxide as the gate dielectric and polysilicon as the gate material. Silicon was implanted into an unintentionally doped GaN layer using the polysilicon gate to define the source and drain regions, with implant activation at 1100/spl deg/C for 5 min in nitrogen. The GaN MOSFETs have a low gate leakage current of less than 50 pA for circular devices with W/L=800/128 /spl mu/m. Devices are normally off with a threshold voltage of +2.7 V and a field-effect mobility of 45 cm/sup 2//Vs at room temperature. The minimum on-resistance measured is 1.9 m/spl Omega//spl middot/cm/sup 2/ with a gate voltage of 34 V (W/L=800/2 /spl mu/m). High-voltage lateral devices had a breakdown voltage of 700 V with gate-drain spacing of 9 /spl mu/m (80 V//spl mu/m), showing the feasibility of self-aligned GaN MOSFETs for high-voltage integrated circuits.     

Lateral RESURF MOSFET fabricated on 4H-SiC(0001/sup ~/) C-face

Lateral reduced surface field (RESURF) metal-oxide-semiconductor field-effect transistors (MOSFETs) have been fabricated on 4H-SiC(0001/sup ~/) carbon face (C-face) substrates. The channel mobility of a lateral test MOSFET on a C-face was 41 cm/sup 2//V/spl middot/s, which was much higher than 5 cm/sup 2//V/spl middot/s for that on a Si-face. The specific on-resistance of the lateral RESURF MOSFET on a C-face was 79/spl Omega/ /spl middot/ cm/sup 2/, at a gate voltage of 25 V and drain voltage of 1 V. The breakdown voltage was 460 V, which was 79% of the designed breakdown voltage of 600 V. We measured the temperature dependence of R/sub on, sp/ for the RESURF MOSFET on the C-face. The R/sub on, sp/ increased with the increase in temperature.     

GaAs MOSFET using InAlP native oxide as gate dielectric

GaAs metal-oxide-semiconductor field-effect transistors (MOSFETs) using wet thermally oxidized InAlP as the gate insulator are reported for the first time. Leakage current measurements show that the 11-nm-thick native oxide grown from an In/sub 0.49/Al/sub 0.51/P layer lattice-matched to GaAs has good insulating properties, with a measured leakage current density of 1.39/spl times/10/sup -7/ mA//spl mu/m/sup 2/ at 1 V bias. GaAs MOSFETs with InAlP native gate oxide have been fabricated with gate lengths from 7 to 2 /spl mu/m. Devices with 2-/spl mu/m-long gates exhibit a peak extrinsic transconductance of 24.2 mS/mm, an intrinsic transconductance of 63.8 mS/mm, a threshold voltage of 0.15 V, and an off-state gate-drain breakdown voltage of 21.2 V. Numerical Poisson's equation solutions provide close agreement with the measured sheet resistance and threshold voltage.     

On the scaling limit of ultrathin SOI MOSFETs

In this paper, a detailed study on the scaling limit of ultrathin silicon-on-insulator (SOI) MOSFETs is presented. Due to the penetration of lateral source/drain fields into standard thick buried oxide, the scale-length theory does not apply to thin SOI MOSFETs. An extensive two-dimensional device simulation shows that for a thin gate insulator, the minimum channel length can be expressed as L/sub min//spl ap/4.5(t/sub Si/+(/spl epsiv//sub Si///spl epsiv//sub I/)t/sub I/), where t/sub Si/ is the silicon thickness, and /spl epsiv//sub I/ and t/sub I/ are the permittivity and thickness of the gate insulator. With t/sub Si/ limited to /spl ges/ 2 nm from quantum mechanical and threshold considerations, a scaling limit of L/sub min/=20 nm is projected for oxides, and L/sub min/=10 nm for high-/spl kappa/ dielectrics. The effect of body doping has also been investigated. It has no significant effect on the scaling limit.     

Lateral power MOSFET for megahertz-frequency, high-density DC/DC converters

DC/DC converters to power future CPU cores mandate low-voltage power metal-oxide semiconductor field-effect transistors (MOSFETs) with ultra low on-resistance and gate charge. Conventional vertical trench MOSFETs cannot meet the challenge. In this paper, we introduce an alternative device solution, the large-area lateral power MOSFET with a unique metal interconnect scheme and a chip-scale package. We have designed and fabricated a family of lateral power MOSFETs including a sub-10 V class power MOSFET with a record-low R/sub DS(ON)/ of 1m/spl Omega/ at a gate voltage of 6V, approximately 50% of the lowest R/sub DS(ON)/ previously reported. The new device has a total gate charge Q/sub g/ of 22nC at 4.5V and a performance figures of merit of less than 30m/spl Omega/-nC, a 3/spl times/ improvement over the state of the art trench MOSFETs. This new MOSFET was used in a 100-W dc/dc converter as the synchronous rectifiers to achieve a 3.5-MHz pulse-width modulation switching frequency, 97%-99% efficiency, and a power density of 970W/in/sup 3/. The new lateral MOSEFT technology offers a viable solution for the next-generation, multimegahertz, high-density dc/dc converters for future CPU cores and many other high-performance power management applications.     

An advanced no-snapback LDMOSFET with optimized breakdown characteristics of drain n-n/sup +/ diodes

Snapbacks in sustain characteristics of lateral double-diffused MOSFETs (LDMOSFETs) are caused by positive feedbacks between the turn-on of the bipolar junction transistors (BJTs) and the avalanche breakdown of the drain n-n/sup +/ diodes . Although the n-n/sup +/ diodes are thus one of the most basic parasitic devices, which play a leading role in the snapback characteristics, neither a textbook nor a paper has ever described their breakdown characteristics in depth so as to realize a simple no-snapback LDMOSFET. This paper analyzes the snapback characteristics of n-n/sup +/ diodes and their mechanisms in detail. The no-snapback theory derived from this study is applied to an advanced no-snapback LDMOSFET with a simple structure, as an improved version of the conventional no-snapback LDMOSFET , which endures the electrostatic discharge (ESD) criterion for automotive applications: 15 kV, 150 pF, and 150 /spl Omega/.     

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     

A new, high-voltage 4H-SiC lateral dual sidewall Schottky (LDSS) rectifier: theoretical investigation and analysis

In this paper, we report a new 4 H-silicon carbide (SiC) lateral dual sidewall Schottky (LDSS) rectifier on a highly doped drift layer consisting of a high-barrier sidewall Schottky contact on top of the low-barrier Schottky contact. Using two-dimensional (2-D) device simulation, the performance of the proposed device has been evaluated in detail by comparing its characteristics with those of the compatible lateral conventional Schottky (LCS) and lateral trench sidewall Schottky (LTSS) rectifiers on 4H-SiC. From our simulation results, it is observed that the proposed LDSS rectifier acts as a low-barrier LTSS rectifier under forward-bias conditions, and as a high-barrier LTSS rectifier under reverse-bias conditions, making it an ideal rectifier. The LDSS rectifier exhibits an on/off current ratio (at 1 V/-500 V) of 5.5/spl times/10/sup 7/ for an epitaxial layer doping of 1/spl times/10/sup 17/ /cm/sup 3/. Further, the proposed LDSS structure exhibits a very sharp breakdown similar to that of a p-i-n diode in spite of using only Schottky junctions in the structure. We have analyzed the reasons for the improved performance of the LDSS.     

High breakdown Voltage undoped AlGaN-GaN power HEMT on sapphire substrate and its demonstration for DC-DC converter application

Undoped AlGaN-GaN power high electron mobility transistors (HEMTs) on sapphire substrate with 470-V breakdown voltage were fabricated and demonstrated as a main switching device for a high-voltage dc-dc converter. The fabricated power HEMT realized a high breakdown voltage with a field plate structure and a low on-state resistance of 3.9 m/spl Omega//spl middot/cm/sup 2/, which is 10 /spl times/ lower than that of conventional Si MOSFETs. The dc-dc converter operation of a down chopper circuit was demonstrated using the fabricated device at the input voltage of 300 V. These results show the promising possibilities of the AlGaN-GaN power HEMTs on sapphire substrate for future switching power devices.     

Lateral n-channel inversion mode 4H-SiC MOSFETs

Advances in MOS devices on silicon carbide (SiC) have been greatly hampered by the low inversion layer mobilities. In this paper, the electrical characteristics of lateral n-channel MOSFETs fabricated on 4H-SiC are reported for the first time. Inversion layer electron mobilities of 165 cm²/V·s in 4H-SiC MOSFETs were measured at room temperature. These MOSFETs were fabricated using a low temperature deposited oxide, with subsequent oxidation anneal, as the gate dielectric     

Edge breakdown in 4H-SiC avalanche photodiodes

We report suppression of edge breakdown in mesa-structure SiC avalanche photodiodes (APDs) by employing a 10/spl deg/ sidewall bevel. These devices exhibit low dark currents, <10 pA for a 160-/spl mu/m-diameter device, at the onset of avalanche gain. Two-dimensional raster scans of both beveled and nonbeveled devices, fabricated from the same wafer, show the photocurrent as a function of position and illustrate the spatial properties of avalanche gain in SiC APDs.     

Impact of switching frequencies on the TID response of SiC power MOSFETs

Different switching frequencies are required when SiC metal-oxide-semiconductor field-effect transistors(MOSFETs)are switching in a space environment.In this study,the total ionizing dose(TID)responses of SiC power MOSFETs are investig-ated under different switching frequencies from 1 kHz to 10 MHz.A significant shift was observed in the threshold voltage as the frequency increased,which resulted in premature failure of the drain-source breakdown voltage and drain-source leakage current.The degradation is attributed to the high activation and low recovery rates of traps at high frequencies.The results of this study suggest that a targeted TID irradiation test evaluation method can be developed according to the actual switching fre-quency of SiC power MOSFETs.     

Low-loss, high-voltage 6H-SiC epitaxial p-i-n diode

The p-i-n diodes were fabricated using 31 /spl mu/m thick n/sup -/- and p-type 6H-SiC epilayers grown by horizontal cold-wall chemical vapor deposition (CVD) with nitrogen and aluminum doping, respectively. The diode exhibited a very high breakdown voltage of 4.2 kV with a low on-resistance of 4.6 m/spl Omega/cm/sup 2/. This on-resistance is lower (by a factor of five) than that of a Si p-i-n diode with a similar breakdown voltage. The leakage current density was substantially lower even at high temperatures. The fabricated SiC p-i-n diode showed fast switching with a turn-off time of 0.18 /spl mu/s at 300 K. The carrier lifetime was estimated to be 0.64 /spl mu/s at 300 K, and more than 5.20 /spl mu/s at 500 K. Various characteristics of SiC p-i-n diodes which have an advantage of lower power dissipation owing to conductivity modulation were investigated.     

A 2K/spl times/8-bit static MOS RAM with a new memory cell structure

A 2K/spl times/8-bit static MOS RAM with a new memory cell structure has been developed. The memory cell consists of six devices including four MOSFETs and two memory load resistors. Two load resistors are fabricated in the second-level polysilicon films over the polysilicon gate MOSFET used as the driver. Thus the memory cell area is determined only by the area of four MOSFETs. By applying the new cell structure and photolithography technology of 3 /spl mu/m dimensions, the cell area of 23/spl times/27 /spl mu/m and the chip area of 3.75/spl times/4.19 mm have been realized. The RAM is nonclocked and single 5 V operation. Access time of about 150 ns is obtained at a supply current of 120 mA.     

Impact of the gate driver voltage on temperature sensitive electrical parameters for condition monitoring of SiC power MOSFETs

Condition monitoring using temperature sensitive electrical parameters (TSEPs) is widely recognized as an enabler for health management of power modules. The on-state resistance/forward voltage of MOSFETs, IGBTs and diodes has already been identified as TSEPs by several researchers. However, for SiC MOSFETs, the temperature sensitivity of on-state voltage/resistance varies depending on the device and is generally not as high as in silicon devices. Recently the turn-on current switching rate has been identified as a TSEP in SiC MOSFETs, but its temperature sensitivity was shown to be significantly affected by the gate resistance. Hence, an important consideration regarding the use of TSEPs for health monitoring is how the gate driver can be used for improving the temperature sensitivity of determined electrical parameters and implementing more effective condition monitoring strategies. This paper characterizes the impact of the gate driver voltage on the temperature sensitivity of the on-state resistance and current switching rate of SiC power MOSFETs. It is shown that the temperature sensitivity of the switching rate in SiC MOSFETs increases if the devices are driven at lower gate voltages. It is also shown, that depending on the SiC MOSFET technology, reducing the gate drive voltage can increase the temperature sensitivity of the on-state resistance. Hence, using an intelligent gate driver with the capability of customizing occasional switching pulses for junction temperature sensing using TSEPs, it would be possible to implement condition monitoring more effectively for SiC power devices.     

Fully depleted dual-gated thin-film SOI P-MOSFETs fabricated in SOI islands with an isolated buried polysilicon backgate

P-channel dual-gated thin-film silicon-on-insulator (DG-TFSOI) MOSFETs have been fabricated with an isolated buried polysilicon backgate in an SOI island formed by epitaxial lateral overgrowth (ELO) of silicon. This structure allows individual operation of both the top and back gates rather than the conventional common backgate structure. When fully-depleted, the buried gate is used to individually shift the top gate threshold voltage (V/sub T/). A linear shift of /spl Delta/V/sub T,top///spl Delta/V/sub G,back/ of 0.5 V/V was achieved with a thin buried oxide. The effective density of interface traps (D/sub it/) for the backgate polysilicon-oxide SOI interface was measured to be 1.8/spl times/10/sup 11/ #/cm/sup 2//spl middot/eV as compared to the substrate-oxide of 1.1/spl times/10/sup 11/ #/cm/sup 2//spl middot/eV.