Electrical characterization of annealed Ti/TiN/Pt contacts onN-type 6H-SiC epilayer

We report results of the electrical characteristics of in vacuo deposited Ti/TiN/Pt contact metallization on n-type 6H-SiC epilayer as function of impurity concentration in the range of 3.3×10¹⁷ cm^-3 to 1.9×10¹⁹ cm^-3. The as-deposited contacts are rectifying, except for the highly doped sample. Only the lesser doped remains rectifying after samples are annealed at 1000°C between 0.5 and 1 min in argon. Bulk contact resistance ranging from factors of 10^-5 to 10^-4 Ω-cm² and Schottky barrier height in the range of 0.54-0.84 eV are obtained. Adhesion problems associated with metal deposition on pre-processed titanium is not observed, leading to excellent mechanical stability. Auger electron spectroscopy (AES) reveals the out diffusion of Ti-Si and agglomeration of Ti-C species at the epilayer surface. The contact resistance remains appreciably stable after treatment in air at 650°C for 65 h. The drop in SBH and the resulting stable contact resistance is proposed to be associated with the thermal activation of TiC diffusion barrier layer on the 6H-SiC epilayer during annealing     

High-voltage Ni- and Pt-SiC Schottky diodes utilizing metal fieldplate termination

We have fabricated 1 kV 4H and 6H SiC Schottky diodes utilizing a metal-oxide overlap structure for electric field termination. This simple structure when used with a high barrier height metal such as Ni has consistently given us good yield of Schottky diodes with breakdown voltages in excess of 60% of the theoretically calculated value. This paper presents the design considerations, the fabrication procedure, and characterization results for these 1 kV Ni-SiC Schottky diodes. Comparison to similarly fabricated Pt-SiC Schottky diodes is reported. The Ni-SiC ohmic contact formation has been studied using Auger electron spectroscopy and X-ray diffraction. The characterization study includes measurements of current-voltage (I-V) temperature and capacitance-voltage (C-V) temperature characteristics. The high-temperature performance of these diodes has also been investigated. The diodes show good rectifying behavior with ON/OFF current ratios, ranging from 10⁶ to 10 at 27°C and in excess of 10⁶ up to 300°C     

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     

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     

Au/Pt/Ti/Ni ohmic contacts to p-ZnTe

Ohmic contacts of Au/Pd/Ti/Ni to p-ZnTe show a minimum specific contact resistance of 10^-6 Ωcm² for a p-type doping level of 3×10¹⁹ cm^-3 and at an annealing temperature of 300°C. The Ni and Ti layers are very effective in improving the electrical properties of these contact     

Electrical properties of Si p+-n junctions for sub-0.25μm CMOS fabricated by Ga FIB implantation

p⁺-n junction diodes for sub-0.25-μm CMOS circuits were fabricated using focused ion beam (FIB) Ga implantation into n-Si (100) substrates with background doping of N_b=(5-10)×10 ¹⁵ and N_b⁺=(1-10)×10¹⁷ cm^-3. Implant energy was varied from 2 to 50 keV at doses ranging from 1×10¹³ to 1×10¹⁵ cm^-2 with different scan speeds. Rapid thermal annealing (RTA) was performed at either 600 °C or 700°C for 30 s. Diodes fabricated on N_b⁺ with 10-keV Ga⁺ exhibited a leakage current (^I_R) 100× smaller than those fabricated with 50-keV Ga⁺. Tunneling was determined to be the major current transport mechanism for the diodes fabricated on N_b⁺ substrates. An optimal condition for I_R on N_b⁺ substrates was obtained at 15 keV/1×10¹⁵ cm^-2. Diodes annealed at 600°C were found to have an I_R 1000× smaller than those annealed at 700°C. I-V characteristics of diodes fabricated on N_b substrates with low-energy Ga⁺ showed no implant energy dependence. I-V characteristics were also measured as a function of temperature from 25 to 200°C. For diodes implanted with 15-keV Ga ⁺, the cross-over temperatures between I_diff and I_g-r occurred at 106°C for N_b ⁺ and at 91°C for N_b substrates     

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     

High voltage GaN Schottky rectifiers

Mesa and planar GaN Schottky diode rectifiers with reverse breakdown voltages (V_RB) up to 550 and >2000 V, respectively, have been fabricated. The on-state resistance, R_ON , was 6 mΩ·cm² and 0.8 Ω cm² , respectively, producing figure-of-merit values for (V_RB )²/R_ON in the range 5-48 MW·cm^-2 . At low biases the reverse leakage current was proportional to the size of the rectifying contact perimeter, while at high biases the current was proportional to the area of this contact. These results suggest that at low reverse biases, the leakage is dominated by the surface component, while at higher biases the bulk component dominates. On-state voltages were 3.5 V for the 550 V diodes and ⩾15 for the 2 kV diodes. Reverse recovery times were <0.2 μs for devices switched from a forward current density of ~500 A·cm^-2 to a reverse bias of 100 V     

Ohmic contacts on diamond by B ion implantation and Ti-Aumetallization

Low-resistance ohmic contacts have been fabricated on a natural IIb semiconducting diamond crystal and on undoped polycrystalline diamond films by B ion implantation and subsequent metallization with a Ti-Au bilayer metallization. A high B concentration of ~7×10²⁰ cm^-3 at the surface was obtained by ion implantation, a post-implant anneal, and a subsequent chemical removal of the graphite layer that resulted from the radiation damage. A bilayer metallization of Ti followed by Au annealed at 850°C yielded a specific contact resistance value on the order of 10^-6 Ω-cm² for chemical-vapor-deposition-grown polycrystalline films and on the order of 10^-5 Ω-cm² for the semiconducting natural crystal     

Electrical properties of low-temperature pyrolytic SiO2on InP

The first application of a new technique (SiH₄+O₂ at 83-330°C and 2-12 torr) for deposition of SiO₂ on InP is reported. SiO₂ deposited at 150-330°C has breakdown strength of 8-10 MV/cm, resistivity >10¹⁵ Ωcm, and refractive index of 1.45-1.46 comparable to thermal SiO ₂ grown at 1100°C. C/V measurements on Al/SiO₂/InP MIS structures suggest that very low temperature oxides (90-100°C) have the best interfacial properties     

Electrical properties of Ga-implanted Si p+-n shallowjunctions fabricated by low-temperature rapid thermal annealing

p⁺-n shallow-junction diodes were fabricated using on-axis Ga⁶⁹ implantation into crystalline and preamorphized Si, at energies of 25-75 keV for a dose of 1×10¹⁵/cm ², which is in excess of the dosage (2×10¹⁴/cm²) required to render the implanted layer amorphous. Rapid thermal annealing at 550-600°C for 30 s resulted in the solid-phase epitaxial (SPE) regrowth of the implanted region accompanied by high Ga activation and shallow junction (60-130 nm) formation. Good diode electrical characteristics for the Ga implantation into crystalline Si were obtained; leakage current density of 1-1.5 nA/cm² and ideality factor of 1.01-1.03. Ga implantation into preamorphized Si resulted in a two to three times decrease in sheet resistance, but a leakage current density orders of magnitude higher     

1.57 μm strained-layer quantum-well GaInAlAs ridge-waveguidelaser diodes with high temperature (130°C) and ultrahigh-speed (17GHz) performance

The fabrication of GaInAlAs strained-layer (SL) multiple-quantum-well (MQW) ridge-waveguide (RW) laser diodes emitting at 1.57 μm is discussed. Due to an optimized layer structure, a very high characteristic temperature of 90 K was obtained. As a consequence for episide-up mounted devices, the maximum continuous wave (CW)-operation temperature is 130°C. At room temperature, a maximum output power of 47 mW was measured for 600-μm-long lasers with one high-reflection coated facet. The low series resistance of 4 Ω (2 Ω) for 200-μm-(400-μm)-long devices yields an ultrahigh 3-dB bandwidth of 17 GHz. These static and dynamic properties also result from a high internal quantum-efficiency of 0.83 and a high differential gain of 5.5×10^-15 cm²     

Current confinement and leakage currents in planarburied-ridge-structure laser diodes on n-substrate

An electrical device model for the planar buried-ridge-structure laser on n-type substrate is discussed. It takes into account the finite p-type contact resistivity, the two-dimensional current spreading, and the electron leakage current by drift and diffusion. Using this model, the influence of the relevant device parameters on the leakage current in InGaAsP/InP devices emitting at 1.3 μm is investigated. It is shown that leakage currents are negligible at room temperature if the contact stripe width does not exceed the sum of the active region width and the p-type confinement layer thickness, but they increase markedly with broader contact stripes and with contact resistivities above 10^-5 Ω-cm². The most important parameter influencing the leakage currents is the doping level of the P-InP confinement layer. With a p-type doping level of 1×10¹⁸ cm^-3, a p-type contact resistivity below 10^-5 Ω-cm² and a contact stripe width of 6 μm, the model calculations predict a maximum operation temperature exceeding 100°C. This agrees fairly well with experimental data proving that the rather simple planar buried-ridge-structure laser performs as well as more sophisticated devices incorporating current-blocking layers     

Isolation on Si wafers by MeV proton bombardment for RF integratedcircuits

This paper studies issues related with using high energy protons to create local semi-insulating silicon regions on IC wafers for device isolation and realization of high-Q IC inductors. Topics on two approaches, i.e., one using Al as the radiation mask and the other using proton direct-write on wafers were studied. It was shown that Al can effectively mask the proton bombardment of 15 MeV up to the fluence of 10¹⁷ cm^-2. For the unmasking direct write of the proton bombardment, isolation in the silicon wafer can be achieved without damaging active devices if the proton fluence is kept below 1×10¹⁴ cm^-2 with the substrate resistivity level chosen at 140 Ω-cm, or kept at 1×10¹⁵ cm ^-2 with the substrate resistivity level chosen at 15 Ω-cm. Under the above approaches, the 1 h-200°C thermal treatment, which is necessary for device final packaging, still gives enough high resistivity for the semi-insulating regions while recovering somewhat the active device characteristics. For the integrated passive inductor fabricated on the surface of the silicon wafer, the proton radiation improves its Q value     

Formation of cobalt silicided shallow junction using implantinto/through silicide technology and low temperature furnace annealing

This work investigates the shallow CoSi₂ contacted junctions formed by BF₂⁺ and As⁺ implantation, respectively, into/through cobalt silicide followed by low temperature furnace annealing. For p⁺n junctions fabricated by 20 keV BF₂⁺ implantation to a dose of 5×10¹⁵ cm^-2, diodes with a leakage current density less than 2 nA/cm² at 5 V reverse bias can be achieved by a 700°C/60 min annealing. This diode has a junction depth less than 0.08 μm measured from the original silicon surface. For n⁺p junctions fabricated by 40 keV As⁺ implantation to a dose of 5×10¹⁵ cm^-2, diodes with a leakage current density less than 5 nA/cm² at 5 V reverse bias can be achieved by a 700°C/90 min annealing; the junction depth is about 0.1 μm measured from the original silicon surface. Since the As⁺ implanted silicide film exhibited degraded characteristics, an additional fluorine implantation was conducted to improve the stability of the thin silicide film. The fluorine implantation can improve the silicide/silicon interface morphology, but it also introduces extra defects. Thus, one should determine a tradeoff between junction characteristics, silicide film resistivity, and annealing temperature     

Electrical characteristics of TiB2 for ULSI applications

The work function of TiB₂ was measured using Fowler-Nordheim tunneling in MOS capacitors, Schottky diode current measurements, capacitance-voltage techniques, and contact resistance. The resulting data place the Fermi level of TiB₂ about 0.9 eV below the silicon conduction band. Given this barrier height, Schottky diodes of TiB₂/p-Si exhibit ohmic characteristics, but the contact resistance of TiB₂ to n⁺ junctions is an order of magnitude higher than the generally desired value. Boron outdiffusion from TiB₂ into underlying silicon was observed at temperatures of 1000°C and greater. Boron diffusion from TiB₂ into silicon above 1000°C is enhanced compared to the conventionally accepted value of the boron diffusivity     

Frequency capability of strained AlAs/InGaAs resonant tunnellingdiodes

The frequency capabilities of integrated In_0.53Ga_0.47As/AlAs resonant tunnelling diodes have been investigated by successfully tracking their resistive cutoff frequencies when the samples are biased in the negative differential conductance region. The devices exhibit extremely high peak current density (J_p=175 kA cm²) and very low series resistance (6×10^-7 Ωcm²) so that submillimetre wave operation can be expected     

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     

Backgating in pseudomorphic In0.15Ga0.85As/Al0.25Ga0.75As MODFET's with a GaAs:Er buffer layer

A new GaAs:Er buffer layer grown by MBE has been developed which significantly reduces backgating currents (by 3 to 4 orders of magnitude) in pseudomorphic InGaAs/AlGaAs modulation-doped field effect transistors (MODFET's). The buffer layer is highly resistive, in the 10 ²-10⁵ Ω·cm range over the Er-doping range investigated. Presence of internal Schottky barriers resulting from high-density ErAs precipitates has been proposed to he the cause of the high resistivity     

Reliability of AlInAs/GaInAs heterojunction bipolar transistors

The reliability of high-performance AlInAs/GaInAs heterojunction bipolar transistors (HBTs) grown by molecular beam epitaxy (MBE) is discussed. Devices with a base Be doping level of 5×10¹⁹ cm^-3 and a base thickness of approximately 50 nm displayed no sign of Be diffusion under applied bias. Excellent stability in DC current gain, device turn-on voltage, and base-emitter junction characteristics was observed. Accelerated life-test experiments were performed under an applied constant collector current density of 7×10⁴ A/cm² at ambient temperatures of 193, 208, and 328°C. Junction temperature and device thermal resistance were determined experimentally. Degradation of the base-collector junction was used as failure criterion to project a mean time to failure in excess of 10⁷ h at 125°C junction temperature with an associated activation energy of 1.92 eV