Lateral IGBT in thin SOI for high voltage, high speed power IC

A high voltage LIGBT built in ultra-thin silicon-on-insulator (SOI) with a linearly graded doping profile is reported. The highest breakdown voltage of 720 V was measured for an LIGBT built in 0.5 μm SOI with a 4 μm buried oxide. A forward voltage drop of 6 V at 100 Acm^-2 and a turn-off time of 140 ns have been achieved in the same device. Device forward voltage drop is very sensitive to the SOI thickness due to the recombination of carriers at the two silicon-silicon dioxide interfaces. An SOI thickness of 0.5 μm and an n-buffer doped to 10¹⁸ cm^-3 have been found to be a reasonable trade-off between the breakdown voltage and the forward voltage drop     

High voltage 4H-SiC Schottky barrier diodes

Characteristics of 4H-SiC Schottky barrier diodes with breakdown voltages up to 1000 V are reported for the first time. The diodes showed excellent forward I-V characteristics, with a forward voltage drop of 1.06 V at an on-state current density of 100 A/cm². The specific on-resistance for these diodes was found to be low (2×10 ^-3 Ω-cm² at room temperature) and showed a T ^1.6 variation with temperature. Titanium Schottky barrier height was determined to be 0.99 eV independent of the temperature. The breakdown voltage of the diodes was found to decrease with temperature     

Avalanche phenomena in 4H-SiC p-n diodes fabricated by aluminum orboron implantation

Characteristics of p-n junction fabricated by aluminum-ion (Al⁺) or boron-ion (B⁺) implantation and high-dose Al⁺-implantation into 4H-SiC (0001) have been investigated. By the combination of high-dose (4×10¹⁵ cm^-2) Al⁺ implantation at 500°C and subsequent annealing at 1700°C, a minimum sheet resistance of 3.6 kΩ/□ (p-type) has been obtained. Three types of diodes with planar structure were fabricated by employing Al+ or B+ implantation. B ⁺-implanted diodes have shown higher breakdown voltages than Al⁺-implanted diodes. A SiC p-n diode fabricated by deep B+ implantation has exhibited a high breakdown voltage of 2900 V with a low on-resistance of 8.0 mΩcm² at room temperature. The diodes fabricated in this study showed positive temperature coefficients of breakdown voltage, meaning avalanche breakdown. The avalanche breakdown is discussed with observation of luminescence     

Breakdown voltage enhancement of the p-n junction by self-aligneddouble diffusion process through a tapered SiO2 implant mask

The low doping region extension at the edge of the junction curvature is implemented with the self-aligned double diffusion process using a tapered SiO₂ implant mask. The p⁺-p-n diodes fabricated with the proposed double diffusion process have relaxed the surface electric field at the junction curvature and increased the breakdown voltage by 140 V, compared with the cylindrical p-n junction. It is also found that the breakdown voltage of the p⁺ -p-n diodes having the field plate (FP) over the tapered oxide is 500 V, while that of the conventional p-n junction with the FP is 280 V     

Low-temperature fabrication of p+-n diodes with300-Å junction depth

Gas immersion laser doping (GILD) was used to fabricate p⁺ -n diodes with 300-Å junction depth. These diodes exhibit ideality factors of 1.01-1.05 over seven decades of current, reverse leakage current densities ⩽10 nA/cm² at -5-V reverse bias, breakdown voltages above 100 V, and electrical activation of the boron impurity to concentrations approaching 1×10²¹ atoms/cm³. This behavior is achieved without the use of a furnace or rapid thermal anneal     

Comparison of GaN p-i-n and Schottky rectifier performance

The performance of GaN p-i-n and Schottky rectifiers fabricated on the same wafer was investigated as a function of device size and operating temperature. There was a significant difference in reverse breakdown voltage (490 V for p-i-n diodes; 347 V for the Schottky diodes) and forward turn-on voltage (~5 V for the p-i-n diodes; ~3.5 V for the Schottky diodes). Both types of device showed a negative temperature coefficient for reverse breakdown, with value -0.34±0.05 V·K^-1     

A high breakdown-voltage SiCN/Si heterojunction diode forhigh-temperature applications

Cubic crystalline p-SiCN films are deposited on n-Si(100) substrates to form SiCN/Si heterojunction diodes (HJDs) with a rapid thermal chemical vapor deposition (RTCVD) technique. The developed SiCN/Si HJDs exhibit good rectifying properties up to 200°C. At room temperature, the reverse breakdown voltage is more than 29 V at the leakage current density of 1.2×10^-4 A/cm². Even at 200°C, the typical breakdown voltage of SiCN/Si HJDs is still preserved about 5 V at the leakage current density of 1.47×10^-4 A/cm². These properties are better than the β-SiC on Si HJDs for high temperature applications     

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     

Experimental determination of electron drift velocity in 4H-SiC p+-n-n+ avalanche diodes

4H-SiC p⁺-n-n⁺ diodes of low series resistivity (<1×10^-4 Ω·cm²) were fabricated and packaged. The diodes exhibited homogeneous avalanche breakdown at voltages U_b=250-270 V according to the doping level of the n layer. The temperature coefficient of the breakdown voltage was measured to be 2.6×10^-4 k^-1 in the temperature range 300 to 573 K. These diodes were capable of dissipating a pulsed power density of 3.7 MW/cm² under avalanche current conditions. The transient thermal resistance of the diode was measured to be 0.6 K/W for a 100-ns pulse width, An experimental determination of the electron saturated drift velocity along the c-axis in 4H-SIC was performed for the first time, It was estimated to be 0.8×10⁷ cm/s at room temperature and 0.75×10⁷ cm/s at approximately 360 K     

Study of bulk and elementary screw dislocation assisted reversebreakdown in low-voltage (<250 V) 4H-SiC p+-n junctiondiodes. II. Dynamic breakdown properties

For Part I see ibid., vol.46, no.3, pp.478-84 (Mar. 1999). This paper outlines the dynamic reverse-breakdown characteristics of low-voltage (<250 V) small-area <5×10^-4 cm² 4H-SiC p⁺-n diodes subjected to nonadiabatic breakdown-bias pulsewidths ranging from 0.1 to 20 μs 4H-SiC diodes with and without elementary screw dislocations exhibited positive temperature coefficient of breakdown voltage and high junction failure power densities approximately five times larger than the average failure power density of reliable silicon pn rectifiers. This result indicates that highly reliable low-voltage SiC rectifiers may be attainable despite the presence of elementary screw dislocations. However, the impact of elementary screw dislocations on other more useful 4H-SiC power device structures, such as high-voltage (>1 kV) pn junction and Schottky rectifiers, and bipolar gain devices (thyristors, ICBT's, etc.) remains to be investigated     

Electrical conduction and dielectric breakdown in aluminum oxideinsulators on silicon

Leakage currents and dielectric breakdown were studied in MIS capacitors of metal-aluminum oxide-silicon. The aluminum oxide was produced by thermally oxidizing AlN at 800-1160°C under dry O₂ conditions. The AlN films were deposited by RF magnetron sputtering on p-type Si (100) substrates. Thermal oxidation produced Al ₂O₃ with a thickness and structure that depended on the process time and temperature. The MIS capacitors exhibited the charge regimes of accumulation, depletion, and inversion on the Si semiconductor surface. The best electrical properties were obtained when all of the AlN was fully oxidized to Al₂O₃ with no residual AlN. The MIS flatband voltage was near 0 V, the net oxide trapped charge density, Q_0x, was less than 10¹¹ cm ^-2, and the interface trap density, D_it, was less than 10¹¹ cm^-2 eV^-1, At an oxide electric field of 0.3 MV/cm, the leakage current density was less than 10^-7 A cm^-2, with a resistivity greater than 10 ¹² Ω-cm. The critical field for dielectric breakdown ranged from 4 to 5 MV/cm. The temperature dependence of the current versus electric field indicated that the conduction mechanism was Frenkel-Poole emission, which has the property that higher temperatures reduce the current. This may be important for the reliability of circuits operating under extreme conditions. The dielectric constant ranged from 3 to 9. The excellent electronic quality of aluminum oxide may be attractive for field effect transistor applications     

High performance of high-voltage 4H-SiC Schottky barrier diodes

High performance of high-voltage rectifiers could be realized utilizing 4H-SiC Schottky barrier diodes. A typical specific on-resistance (R_on) of these devices was 1.4×10³ Ω cm³ at 24°C (room temperature) with breakdown voltages as high as 800 V. These devices based on 4H-SiC had R _on's lower than 6H-SiC based high-power rectifiers with the same breakdown voltage. As for Schottky contact metals, Au, Ni, and Ti were employed in this study. The barrier heights of these metals for 4H-SiC were determined by the analysis of current-voltage characteristics, and the reduction of power loss could be achieved by controlling the barrier heights     

Process and device characterization of high voltage gallium arsenide P-i-N layers grown by an improved liquid phase epitaxy method

GaAs P-i-N layers with an i-region net doping of less than 10¹² cm⁻³ were grown on P⁺ and N⁺ substrates by a modified liquid phase epitaxy (LPE) method. Doping profiles and structural data obtained by varius characterization techniques are presented and discussed. A P⁺-P-i-N-N⁺ diode with a 25 μm-wide i-region exhibits a breakdown voltage of 1000 V, a t_rr of 50 ns, and reverse current densities (at V_R = 800 V) of − 3 × 10⁻⁶ A/cm² at 25°C and 10⁻² A/cm² at 260° C.     

Turn-on process in 4H-SiC thyristors

Detailed turn-on measurements of 4H-Silicon Carbide (SiC) npnp thyristors are presented for a wide range of operating conditions. Comparisons with similarly-rated silicon and Gallium Arsenide thyristors show a superior rise time and pulsed turn-on performance of SiC thyristors. Rise time for a 400 V blocking voltage, 4 V forward drop (2.8×10³ A/cm²) SiC thyristor has been found to be of the order of 3-5 ns. Pulsed turn on measurements show a residual voltage of only 50 V when a current density of 10⁵ A/cm² (35 A) was achieved in 20 ns     

Characteristics of planar n-p junction diodes made bydouble-implantations into 4H-SiC

Double implantation technology consisting of deep-range acceptor followed by shallow-range donor implantation was used to fabricate planar n⁺-p junction diodes in 4H-SiC. Either Al or B was used as the acceptor species and N as the donor species with all implants performed at 700°C and annealed at 1650°C with an AlN encapsulant. The diodes were characterized for their current-voltage (I-V) and capacitance-voltage (C-V) behavior over the temperature range 25°C-400°C, and reverse recovery transient behavior over the temperature range 25°C-200°C. At room temperature, the B-implanted diodes exhibited a reverse leakage current of 5×10^-8 A/cm² at a reverse bias of -20 V and a carrier lifetime of 7.4 ns     

Increasing the current density of dielectric-base transistors withan MgO emitter-base barrier

We measured the current-voltage characteristics of YBa₂Cu₃O_7-x/oxide/n-SrTiO₃ diodes using NdGaO₃, LaAlO₃, CeO₂, and MgO as the oxide. MgO films had the highest current density. We then fabricated dielectric-base transistors with a YBa₂Cu₃ O_7-x(YBCO) emitter/collector on a SrTiO₃ dielectric base with an MgO barrier. The transistors had both voltage and current gains exceeding unity at 4.2 K. The emitter current density was about 4×10³ A/cm² at a collector-emitter voltage of 10 V and base-emitter voltage 10 V; this is 2 to 3 orders of magnitude larger than that of transistors with NdGaO₃ emitter-base barrier. We obtained a transconductance of around 0.4 mS at a collector-emitter voltage of 10 V for a device with a 6-μm-diameter emitter     

P-type 4H and 6H-SiC high-voltage Schottky barrier diodes

High-voltage Schottky barrier diodes have been successfully fabricated for the first time on p-type 4H- and 6H-SiC using Ti as the barrier metal. Good rectification was confirmed at temperatures as high as 250°C. The barrier heights were estimated to be 1.8-2.0 eV for 6H-SiC and 1.1-1.5 eV for 4H-SiC at room temperature using both I-V and C-V measurements. The specific on resistance (R_on,sp) for 4H- and 6H-SiC were found to be 25 mΩ cm^-2 and 70 mΩ cm^-2 at room temperature. A monotonic decrease in resistance occurs with increasing temperature for both polytypes due to increased ionization of dopants. An analytical model is presented to explain the decrease of R_on,sp with temperature for both 4H and 6H-SiC which fits the experimental data. Critical electric field strength for breakdown was extracted for the first time in both p-type 4H and 6H-SiC using the breakdown voltage and was found to be 2.9×10⁶ V/cm and 3.3×10⁶ V/cm, respectively. The breakdown voltage remained fairly constant with temperature for 4H-SiC while it was found to decrease with temperature for 6H-SiC     

Analytical solutions for the breakdown voltages of punched-through diodes having curved junction boundaries at the edges

Analytical expressions are derived for the breakdown voltages of punched-through diodes having a plane structure terminated with cylindrical and spherical curved boundaries at the edges, through the use of suitable approximations for the electric field in the depletion layer. The expressions derived include both p⁺-i-n⁺and p⁺-p-n⁺(or p⁺-n-n⁺) types and are given in terms of the middle-region (i-layer or p-layer) width, the radius of curvature of the junction edge, the punch-through voltage, and the plane parallel breakdown voltage of p⁺-i-n⁺diodes. The results obtained include a correlation between the middle-region (p-layer) width and the width of the depletion layer in the curved portions of the junction when the applied reverse bias across the diode is just sufficient so that punchthrough takes in the portions where the junction is plane parallel. These results are made use of in the breakdown voltage calculations.     

Extrapolation of high-voltage stress measurements to low-voltageoperation for thin silicon-oxide films

Breakdown and wearout in MOS capacitors fabricated with 10 nm-thick silicon oxide films on p-type silicon are discussed. They have been stressed at high voltages. The high-voltage-stress-induced changes in the oxide properties are extrapolated to low operating voltages. The stress voltages ranged from -7.5 V to -14.5 V. The fluence during the stress was systematically varied front 2×10^-5 C/cm² to 6 C/cm² by varying the stress time at each voltage. The number of interface traps generated by the stress increased as the stress voltage and fluence increased. However, the interface trap generation rate decreased as the fluence increased. The trap generation rate at low operating voltages was very high, but because the current through the oxide was small, the total number of traps generated was low. The trap generation rate was proportional to the inverse square root of the fluence with a voltage dependence that decreased as the fluence increased. Extrapolation of the high-voltage-stress measurements to 5 V shows that easily detectable changes in the oxide properties would only occur after several years of 5 V operation. Extrapolation of charge-to-breakdown and time-to-breakdown data to 5 V operation indicates that breakdown would occur after hundreds of years of device operation     

4H-SiC TSOB结势垒肖特基二极管静态特性

为增强器件的反向耐压能力,降低器件的漏电功耗,采用Silvaco TCAD对沟槽底部具有SiO₂间隔的结势垒肖特基二极管(TSOB)的器件特性进行了仿真研究。通过优化参数来改善导通压降(V_F)-反向漏电流(I_R)和击穿电压的折衷关系。室温下,沟槽深度为2.2 μm时,器件的击穿电压达到1 610 V。正向导通压降为2.1 V,在V_F=3 V时正向电流密度为199 A/cm²。为进一步改善器件的反向阻断特性,在P型多晶硅掺杂的有源区生成一层SiO₂来优化漂移区电场分布,此时改善的器件结构在维持正向导通压降2.1 V的前提下,击穿电压达到1 821 V,增加了13%。在1 000 V反向偏置电压下,反向漏电流密度比普通结构降低了87%,有效降低了器件的漏电功耗。普通器件结构的开/关电流比为2.6×10³(1 V/-500 V),而改善的结构为1.3×10⁴(1 V/-500 V)。