Interface characteristics of Ge3N4-(n-type) GaAs MIS devices

Passivation of GaAs surfaces was achieved by the deposition of Ge₃N₄ dielectric films at low temperatures. Electrical characteristics of MIS devices were measured to determine the interface parameters. From C-V-f and G-V-f measurements, density of interface states has been obtained as (4–6)×10¹¹ cm⁻² eV⁻¹ at the semiconductor mid-gap. Some inversion charge buildup was seen in the C-V plot although the strong inversion regime is absent. Thermally stimulated current measurements indicate a trap density of 5×10¹⁸−10¹⁹ cm⁻³ in the dielectric film, with their energy level at 0.59 eV.     

GaN p–n junction diode formed by Si ion implantation into p-GaN

²⁸Si⁺ implantation into Mg-doped GaN, followed by thermal annealing in N₂ was performed to achieve n⁺-GaN layers. The carrier concentrations of the films changed from 3×10¹⁷ (p-type) to 5×10¹⁹ cm⁻³ (n-type) when the Si-implanted p-type GaN was properly annealed. Specific contact resistance (ρ_c) of Ti/Al/Pt/Au Ohmic contact to n-GaN, formed by ²⁸Si⁺ implantation into p-type GaN, was also evaluated by transmission line model. It was found that we could achieve a ρ_c value as low as 1.5×10⁻⁶ Ω cm² when the metal contact was alloyed in N₂ ambience at 600 °C. Si-implanted GaN p–n junction light-emitting diodes were also fabricated. Electroluminescence measurements showed that two emission peaks at around 385 and 420 nm were observed, which could be attributed to the near band-edge transition and donor-to-acceptor transition, respectively.     

Ohmic contacts for GaAs devices

Contact alloys were developed for use on a wide variety of GaAs devices such as high temperature transistors and Gunn oscillators. The alloys are composed of silver, indium and germanium for n-type GaAs and of silver, indium and zinc for p-type GaAs. Fabrication steps that require temperatures of up to 770°K for already contacted devices can be performed. GaAs transistors can be operated over a range from 20 to 770°K using Ag-In-Ge contacts for emitter and collector and Ag-In-Zn contacts for the base. Gunn oscillators have been built for the frequency range between 13 and 26 GHz with efficiencies as high as 3 percent at 15.8 GHz and as high as 1 percent at 25 GHz in continuous wave operation. A simple technique was developed to evaluate the specific contact resistance on thin epitaxial layers. Specific contact resistance is well below 10⁻⁴ ω-cm² on 0.1 ω-cm or lower resistivity p- or n-type GaAs. The highest value was 1 × 10⁻³ ω-cm² measured on 0.6–2.6 ω-cm n-type GaAs.     

An investigation of LixNi1−x,O as a mixed-valence thermoelectric material

The mixed valence material, Li_xNi_1−xO, has been investigated as a potential thermoelectric material. Measurements of the Seebeck coefficient, (μ V/°C), electrical resistivity, ρ(Ω-cm), and thermal conductivity, k(W/cm°C) have been made as a function of temperature and lithium concentration. The thermoelectric figure of merit, Z(²/ρk), reaches a value of approximately 1·4×10⁻⁴ at 1100°C for the composition Li_0.04Ni_0.96O.     

On the electrical resistivity and chemical etching of TiSi2 thin films sputtered from a composite target

The electrical resistivity of TiSi₂ thin films sputtered onto an oxidised Si substrate using a composite alloy target is studied. It is found that the as-deposited films show high resistivity. Annealing the films at an elevated temperature leads to a significant fall in the resistivity. An optimum sheet resistance of 2om tq⁻¹ is obtained after annealing at 800°C for 30 min in argon ambient. The effect of annealing temperature on resistivity is studied. The sheet resistance is also found to be affected by the magnitude of the substrate bias during film deposition. The data are given. The patterning of TiSi₂ thin films by wet chemical etching for device applications is described.     

Schottky barrier height of a new ohmic contact NiSi2 to n-type 6H-SiC

We present a new ohmic contact material NiSi₂ to n-type 6H-SiC with a low specific contact resistance. NiSi₂ films are prepared by annealing the Ni and Si films separately deposited on (0 0 0 1)-oriented 6H-SiC substrates with carrier concentrations (n) ranging from 5.8×10¹⁶ to 2.5×10¹⁹ cm⁻³. The deposited films are annealed at 900 °C for 10 min in a flow of Ar gas containing 5 vol.% H₂ gas. The specific contact resistance of NiSi₂ contact exponentially decreases with increasing carrier concentrations of substrates. NiSi₂ contacts formed on the substrates with n=2.5×10¹⁹ cm⁻³ show a relatively low specific contact resistance with 3.6×10⁻⁶ Ω cm². Schottky barrier height of NiSi₂ to n-type 6H-SiC is estimated to be 0.40±0.02 eV using a theoretical relationship for the carrier concentration dependence of the specific contact resistance.     

CoSi2 ohmic contacts to n-type 6H---SiC

Cobalt disilicide (CoSi₂) ohmic contacts possessing low specific contact resistivity (_c < 3.0 ± 0.4 × 10⁻⁵ ωcm²) to n-type 6H---SiC are reported. The contacts were fabricated via sequential electron-beam evaporation of Co and Si layers followed by a two-step vacuum anealing process at 500 and 900°C. Stochiometry of the contact so formed was confirmed by Rutherford backscattering spectrometry and X-ray diffraction. Specific contact resistivities were obtained via current-voltage (I-V) analysis at temperatures ranging from 25 to 500°C. _c is compared as a function of carrier concentration, current density, temperature and time at elevated temperature.     

The self-formatting barrier characteristics of Cu–Mg/SiO2 and Cu–Ru/SiO2 films for Cu interconnects

To substitute or to supplement diffusion barrier as reducing lateral dimension of interconnects, the alloying Mg and Ru to Cu was investigated as a self-formatting barrier in terms of their resistivity, adhesion, and barrier characteristics After annealing at 400 °C for 30 min, the resistivities of the Cu–0.7 at%Mg alloy and Cu–2.2 at%Ru alloy were 2.0 μΩ cm and 2.5 μΩ cm, respectively, which are comparable to that of Cu films. The adhesion was investigated by means of a sandwiched structure using the four point bending test. The interfacial debonding energy, which represents the adhesion, of Cu–Mg/SiO₂ was over 5.0 J/m², while those of the Cu–Ru/SiO₂ and Cu/SiO₂ interfaces were 2.2 J/m² and 2.4 J/m², respectively. The barrier characteristics of the alloy films were also investigated by the time-dependent dielectric breakdown test, using a metal–oxide–semiconductor structure, under bias-temperature stress. It was shown that the alloying of Mg made the lifetime seven times longer, as opposed to the alloying of Ru which made it shorter.     

Characterization of phosphorus implanted low pressure chemical vapor deposited polycrystalline silicon

Thin (3000–5000Å) low pressure chemically vapor deposited (LPCVD) films of polycrystalline silicon suitable for microelectronics applications have been deposited from silane at 600°C and at a pressure of 0.25 Torr. The films were phosphorus implanted at 150 KeV and electrically characterized with the annealing conditions and film thickness as parameters, over a resistivity range of four orders of magnitude (10³–10⁷Ω/□). Annealing during silox deposition was found to result in a lower film resistivity than annealing done in nitrogen atmosphere. Resistivity measurements as a function of temperature indicate that the electrical activation energy is a linear function of 1/N(N is the doping concentration), changing from 0.056 eV for a doping concentration of 8.9 × 10¹⁸ cm⁻³ to 0.310 eV for doping concentration of 3.3 × 10¹⁸ cm⁻³. The grain boundary trap density was found to have a logarithmically decreasing dependence on the polysilicon thickness, decreasing from 1.3 × 10¹³ cm⁻² for 2850Å polysilicon film to 8.3 × 10¹² cm⁻² for 4500Å polysilicon film.     

High-κ Al2O3−HfTiO Nanolaminates With Less Than 0.8-nm Equivalent Oxide Thickness

High quality nanolaminate stacks consisting of five Al₂O₃-HfTiO layers with an effective dielectric constant of about 22.5 are reported. A dielectric constant for binary HfTiO thick films of about 83 was also demonstrated. The electrical characteristics of as-deposited structures and ones which were annealed in an O₂ atmosphere at up to 950 degC for 5-10 min were investigated. Two types of gate electrodes: Pt and Ti were compared. The dielectric stack which was annealed up to 500 degC exhibits a leakage current density as small as ~1times10^-4 A/cm² at an electric of field 1.5 MV/cm for a quantum-mechanical corrected equivalent oxide thickness of ~0.76 nm. These values change to ~1times10^-8 A/cm² and 1.82 nm, respectively, after annealing at 950 degC     

Stability of hydrogen in ScAlMgO4

Hydrogen as ²H was incorporated into ScAlMgO₄ by both ion implantation and by exposure to a plasma at 250°C. In the implanted material diffusion begins at 500°C and most of the hydrogen is lost by ≤ 750°C. This thermal stability for hydrogen retention is considerably lower than for other substrate materials for GaN epilayer growth, such as Al₂O₃ and SiC. There is minimal permeation of ²H from a plasma at 250°C (D_H ≤ 5 × 10⁻¹⁶ cm² s⁻¹) in ScAlMgO₄, and thus unintentional hydrogen incorporation into GaN overlayers should be minimal at typical growth temperatures.     

Transport properties of Mn-doped Ru2Si3

Transport properties of Mn-doped ruthenium silicide Ru₂Si₃ were studied both experimentally and theoretically. The precipitation-free Ru₂Si₃ single crystals were grown by the zone melting technique with radiation heating. The temperature dependence of the electrical resistivity and Hall coefficients of the crystals were measured. The electrical resistivity of 1% Mn-doped Ru₂Si₃ was lower than that of undoped crystals. The carrier concentration in the doped samples is about 10¹⁸ cm⁻³ at room temperature. Mn-doped Ru₂Si₃ has a twice higher carrier mobility compared to the undoped one. Theoretical calculation of the charge carrier mobility is based on the effective masses which are estimated from the ab initio electronic band structure and classical scattering mechanisms.     

High temperature ohmic contacts to 3C–silicon carbide films

Currently, large-area 3C–SiC films are available from a number of sources and it is imperative that stable high temperature contacts be developed for high power devices on these films. By comparing the existing data in the literature, we demonstrate that the contact behavior on each of the different polytypes of SiC will vary significantly. In particular, we demonstrate this for 6H–SiC and 3C–SiC. The interface slope parameter, S, which is a measure of the Fermi-level pinning in each system varies between 0.4–0.5 on 6H–SiC, while it is 0.6 on 3C–SiC. This implies that the barrier heights of contacts to 3C–SiC will vary more significantly with the choice of metal than for 6H–SiC. Aluminum, nickel and tungsten were deposited on 3C–SiC films and their specific contact resistance measured using the circular TLM method. High temperature measurements (up to 400°C) were performed to determine the behavior of these contacts at operational temperatures. Aluminum was used primarily as a baseline for comparison since it melts at 660°C and cannot be used for very high temperature contacts. The specific contact resistance (ρ_c) for nickel at room temperature was 5×10⁻⁴ Ω cm², but increased with temperature to a value of 1.5×10⁻³ Ω cm² at 400°C. Tungsten had a higher room temperature ρ_c of 2×10⁻³ Ω cm², which remained relatively constant with increasing temperature up to 400°C. This is related to the fact that there is hardly any reaction between tungsten and silicon carbide even up to 900°C, whereas nickel almost completely reacts with SiC by that temperature. Contact resistance measurements were also performed on samples that were annealed at 500°C.     

Optoelectronic properties of Zn0.52Se0.48/Si Schottky diodes

Zn_0.52Se_0.48/Si Schottky diodes are fabricated by depositing zinc selenide (Zn_0.52Se_0.48) thin films onto Si(1 0 0) substrates by vacuum evaporation technique. Rutherford backscattering spectrometry (RBS) analysis shows that the deposited films are nearly stoichiometric in nature. X-ray diffractogram of the films reveals the preferential orientation of the films along (1 1 1) direction. Structural parameters such as crystallite size (D), dislocation density (δ), strain (ε), and the lattice parameter are calculated as 29.13 nm, 1.187 × 10⁻¹⁵ lin/m², 1.354 × 10⁻³ lin⁻² m⁻⁴ and 5.676 × 10⁻¹⁰ m respectively. From the I–V measurements on the Zn_0.52Se_0.48/p-Si Schottky diodes, ideality and diode rectification factors are evaluated, as 1.749 (305 K) and 1.04 × 10⁴ (305 K) respectively. The built-in potential, effective carrier concentration (N_A) and barrier height were also evaluated from C–V measurement, which are found to be 1.02 V, 5.907 × 10¹⁵ cm⁻³ and 1.359 eV respectively.     

Long-term bias temperature reliability of P+ polysilicongated FET devices

An instability was found to be associated with +BT stress for P ⁺ poly-gated NMOSFETs (PNMOS) and PMOSFETs (PPMOS), but not with the N⁺ poly-gated devices (NNMOS and NPMOS). The instability with the P⁺ poly-gated devices, which is a decrease in threshold voltage (V_t) and an increase in interface state density (D_it), was significantly reduced following N₂ annealing at 400°C. It is shown that adequate reliability for P⁺ poly-gated devices can be achieved for VLSI technologies     

The intervalley X6→Γ6, L6 scattering time in GaAs measured by ultrafast pump-probe infrared absorption spectroscopy

A direct measurement of the dynamics of electrons in the X₆ valley for a GaAs crystal by time-resolved absorption spectroscopy is reported for the first time. IR picosecond probe pulses were used to monitor the growth and decay of the population in the X₆ valley subsequent to excitation by a 527 nm pump pulse. The intervalley X₆→Γ₆, L₆ scattering time t_x of 0.70 ± 0.50 ps is determined and the crossection for the X₆→X₇ transition is estimated to be 1.8 × 10⁻¹⁶ cm².     

MoSi2formation by rapid isothermal annealing

Formation of MoSi2by rapid isothermal annealing has been investigated using black-body radiation from a graphite heater. Although elemental Mo layers deposited on 3 in diameter silicon wafers failed to form silicides after annealing, excellent results were obtained using co-sputtered Mo and Si on similar substrates. It was found that regrowth began within the first few seconds at 900-1000°C, and a 20 sec anneal time at 1000°C reduces sheet resistivity by one order of magnitude from as-deposited values. This method of annealing might thus offer a practical solution to low-resistivity silicide formation in very large-scale integrated-circuit devices, without the significant dopant redistribution observed in furnace annealing.     

Estimation for the capture cross-sections of surface state on p-Si surface by photovoltaic method

A new method which can nondestructively measure the surface-state density (SSD) D_s and estimate the capture cross-sections (CCS) of surface state σ⁰_n and σ⁻_p on surface of p-type semiconductor crystals is proposed. This method is based on the photovoltage measurements at various temperatures. The photovoltage experiment was carried out with a (1 1 1) p-type Si single crystal (N_A=4.8×10¹⁴ cm ⁻³). Owing to that the surface barrier height φ_BP=0.6421 V and the surface-recombination velocity s_n=9.6×10³ cm s⁻¹ of this sample can be determined, the SSD D_s=1.2×10¹¹ cm⁻² eV⁻¹ can therefore be obtained, furthermore CCS σ⁰_n≈5×10⁻¹⁴ cm² and σ⁻_p≈2×10⁻¹⁰ cm² can also be estimated. These results are consistent with that of related reports obtained by other methods.     

Silicon nano-particles in SiO2 sol–gel film for nano-crystal memory device applications

A novel 2-bit nano-silicon based non-volatile memory is proposed to double memory density. The thin film structure exhibits two conduction states (ON and OFF) at different voltages and has a cost-effective structure. The structure utilizes the good electrical properties of fluorinated SiO₂ thin films, together with the bi-stable properties conferred by the nano-silicon particles therein embedded. A polymeric layer of 8-hydroxyquinoline aluminum salt (Alq3) further deposited on the top of the nano-particle layer through chemical evaporation and a silver paste contact determines the final structure. The positive 0–15 V scan reveals two discontinuities with an ON/OFF ratio of 10⁴–10⁵ (2–4 V) and OFF/ON of 10³ (12.5–13.0 V). The reverse scan displays again two distinct thresholds, range of 10.5–11.0 V (ON/OFF ratio 10⁻³), respectively, 0.5 V (OFF/ON ratio 10⁻⁵–10⁻⁴).     

Effect of bottom electrode materials on the electrical andreliability characteristics of (Ba, Sr)TiO3 capacitors

The dielectric constant and the leakage current density of (Ba, Sr)TiO₃ (BST) thin films deposited on various bottom electrode materials (Pt, Ir, IrO₂/Ir, Ru, RuO₂/Ru) before and after annealing in O₂ ambient were investigated. The improvement of crystallinity of BST films deposited on various bottom electrodes was observed after the postannealing process. The dielectric constant and leakage current of the films mere also strongly dependent on the postannealing conditions. BST thin film deposited on Ir bottom electrode at 500°C, after 700°C annealing in O₂ for 20 min, has the dielectric constant of 593, a loss tangent of 0.019 at 100 kHz, a leakage current density of 1.9×10 ^-8 A/cm² at an electric field of 200 kV/cm with a delay time of 30 s, and a charge storage density of 53 fC/μm² at an applied field of 100 kV/cm. The BST films deposited on Ir with post-annealing can obtain better dielectric properties than on other bottom electrodes in our experiments. And Ru electrode is unstable because the interdiffusion of Ru and Ti occurs at the interface between the BST and Ru after postannealing. The ten year lifetime of time-dependent dielectric breakdown (TDDB) studies indicate that BST on Pt, Ir, IrO₂/Ir, Ru, and RuO₂/Ru have long lifetimes over ten gears on operation at the voltage bias of 2 V