Co gamma irradiation effects on electrical characteristics of Al/Y2O3/n-Si/Al capacitors

Al/Y₂O₃/n-Si/Al capacitors were irradiated by using a ⁶⁰Co gamma ray source and a maximum dose up to 8.4 kGy. The effect of an annealing treatment performed at 600 or 900 °C on the yttrium oxide (Y₂O₃) films was investigated by XRD and Raman spectroscopy. High-frequency capacitance-voltage (C-V) and conductance-voltage (G-V) measurements as well as quasi-static measurements of the MOS structures were analysed. The annealing improves the crystalline state of the Y₂O₃ thin film material and decreases the values of the flat-band voltage and of the interface trap level density indicating an improvement of the electrical properties of the interface thin film-substrate. But at this interface, the formation of an yttrium-silicate layer was also evidenced. After gamma irradiation, the values of the flat-band voltage and of the interface trap level density related to the Al/Y₂O₃/n-Si/Al structure increase and especially for the structure made with the materials annealed at 900 °C for 1 h. In that case, the structure is very sensitive to a gamma irradiation dose up to 8.4 kGy.     

Titanium-aluminum oxynitride (TAON) as high-k gate dielectric for sub-32 nm CMOS technology

High-k insulators for the next generation (sub-32 nm CMOS (complementary metal-oxide-semiconductor) technology), such as titanium-aluminum oxynitride (TAON) and titanium-aluminum oxide (TAO), have been obtained by Ti/Al e-beam evaporation, with additional electron cyclotron resonance (ECR) plasma oxynitridation and oxidation on Si substrates, respectively. Physical thickness values between 5.7 and 6.3 nm were determined by ellipsometry. These films were used as gate insulators in MOS capacitors fabricated with Al electrodes, and they were used to obtain capacitance-voltage (C-V) measurements. A relative dielectric constant of 3.9 was adopted to extract the equivalent oxide thickness (EOT) of films from C-V curves under strong accumulation condition, resulting in values between 1.5 and 1.1 nm, and effective charge densities of about 10¹¹ cm⁻². Because of these results, nMOSFETs with Al gate electrode and TAON gate dielectric were fabricated and characterized by current-voltage (I-V) curves. From these nMOSFETs electrical characteristics, a sub-threshold slope of 80 mV/dec and an EOT of 0.87 nm were obtained. These results indicate that the obtained TAON film is a suitable gate insulator for the next generation (MOS) devices.     

Temperature and frequency dependent electrical and dielectric properties of Al/SiO2/p-Si (MOS) structure

The electrical and dielectric properties of Al/SiO₂/p-Si (MOS) structures were studied in the frequency range 10 kHz-10 MHz and in the temperature range 295-400 K. The interfacial oxide layer thickness of 320 Å between metal and semiconductor was calculated from the measurement of the oxide capacitance in the strong accumulation region. The frequency and temperature dependence of dielectric constant (ε′), dielectric loss (ε″), dielectric loss tangent (tan δ) and the ac electrical conductivity (σ_ac) are studied for Al/SiO₂/p-Si (MOS) structure. The electrical and dielectric properties of MOS structure were calculated from C-V and G-V measurements. Experimental results show that the ε′ and ε″ are found to decrease with increasing frequency while σ_ac is increased, and ε′, ε″, tan δ and σ_ac increase with increasing temperature. The values of ε′, ε″ and tan δ at 100 kHz were found to be 2.76, 0.17 and 0.06, respectively. The interfacial polarization can be more easily occurred at low frequencies, and the number of interface state density between Si/SiO₂ interface, consequently, contributes to the improvement of dielectric properties of Al/SiO₂/p-Si (MOS) structure. Also, the effects of interface state density (N_ss) and series resistance (R_s) of the sample on C-V characteristics are investigated. It was found that both capacitance C and conductance G were quite sensitive to temperature and frequency at relatively high temperatures and low frequencies, and the N_ss and R_s decreased with increasing temperature. This is behavior attributed to the thermal restructuring and reordering of the interface. The C-V and G/ω-V characteristics confirmed that the N_ss, R_s and thickness of insulator layer (δ) are important parameters that strongly influence both the electrical and dielectric parameters and conductivity in MOS structures.     

MOS devices with tetragonal ZrO2 as gate dielectric formed by annealing ZrO2/Ge/ZrO2 laminate

A Ge-stabilized tetragonal ZrO₂ (t-ZrO₂) film with permittivity (κ) of 36.2 was formed by depositing a ZrO₂/Ge/ZrO₂ laminate and a subsequent annealing at 600 °C, which is a more reliable approach to control the incorporated amount of Ge in ZrO₂. On Si substrates, with thin SiON as an interfacial layer, the SiON/t-ZrO₂ gate stack with equivalent oxide thickness (EOT) of 1.75 nm shows tiny amount of hysteresis and negligible frequency dispersion in capacitance-voltage (C-V) characteristics. By passivating leaky channels derived from grain boundaries with NH₃ plasma, good leakage current of 4.8 × 10⁻⁸ A/cm² at V_g = V_fb − 1 V is achieved and desirable reliability confirmed by positive bias temperature instability (PBTI) test is also obtained.     

Analysis of electrical characteristics of Au/SiO2/n-Si (MOS) capacitors using the high-low frequency capacitance and conductance methods

The purpose of this paper is to analyze electrical characteristics in Au/SiO₂/n-Si (MOS) capacitors by using the high-low frequency (C_HF-C_LF) capacitance and conductance methods. The capacitance-voltage (C-V) and conductance-voltage (G/ω-V) measurements have been carried out in the frequency range of 1 kHz-10 MHz and bias voltage range of (−12 V) to (12 V) at room temperature. It was found that both C and G/ω of the MOS capacitor were quite sensitive to frequency at relatively low frequencies, and decrease with increasing frequency. The increase in capacitance especially at low frequencies is resulting from the presence of interface states at Si/SiO₂ interface. Therefore, the interfacial states can more easily follow an ac signal at low frequencies, consequently, which contributes to the improvement of electrical properties of MOS capacitor. The interface states density (N_ss) have been determined by taking into account the surface potential as a function of applied bias. The energy density distribution profile of N_ss was obtained from C_HF-C_LF capacitance method and gives a peak at about the mid-gap of Si. In addition, the high frequency (1 MHz) capacitance and conductance values measured under both reverse and forward bias have been corrected for the effect of series resistance (R_s) to obtain the real capacitance of MOS capacitors. The frequency dependent C-V and G/ω-V characteristics confirm that the N_ss and R_s of the MOS capacitors are important parameters that strongly influence the electrical properties of MOS capacitors.     

The protective effect of thin amorphous hydrogenated carbon a-C:H films during metallisation of metal-carbon-oxide-silicon (MCOS) diodes

Capacitance-voltage (C-V) characteristics of the as-grown metal(Al)-carbon-oxide(SiO₂)-semiconductor(Si) structures are examined at the frequency of 1 MHz and compared with the C-V characteristics of the conventional metal(Al)-SiO₂-Si (MOS) structures. The density of the oxide charge Q_o/q is extracted from the experimental results. Q_o/q was found to be 1×10¹² cm⁻² for the MOS structures and 7×10¹¹ cm⁻² for the metal-carbon-oxide-silicon structures. This difference can be attributed to the presence of the carbon layer which acts as a protective coating during metallisation of the wafers.     

Investigation of 4H-SiC MOS capacitors annealed in diluted N2O at different temperatures

Thermally grown oxide on 4H-SiC has been post-annealed in diluted N₂O (10% N₂O in N₂) at different temperatures from 900 to 1100 °C. The quality of the nitrided oxide and the SiO₂/4H-SiC interface was investigated by AC conductance and high frequency C-V measurements based on Al/SiO₂/4H-SiC metal-insulator-semiconductor (MOS) structure. It is found that N₂O annealing at 1000 °C produces the lowest interface state density, though the difference is not so significant when compared to the other samples annealed at 900 and 1100 °C. These results can be explained by the high temperature dynamic decomposition process of N₂O. By fitting the AC conductance data, it is found that higher temperature nitridation increases the capture cross-section of the interface traps.     

Multilevel charge storage in Si nanocrystals arranged in double-dot-layers within SiO2

We investigated charging/discharging characteristics of a MOS structure with two layers of Si-nanocrystals (NCs) embedded in the SiO₂ dielectric. The two-dimensional (2D) arrays of nanocrystals, of sizes 3 and 5 nm in the lower and upper NCs layer, respectively, were fabricated by low pressure chemical vapor deposition (LPCVD) of amorphous Si (a-Si), followed by oxidation/annealing. The tunnel oxide was 3.5 nm thick. Successive charging of the NCs layers by both electrons and holes injected from the substrate was clearly demonstrated by the observed steps in the flatband voltage shift (ΔV_FB) as a function of the applied positive (electrons) or negative (holes) pulses on the gate, thus opening the potential for multiple bit operation of the memory. Discharging of the structure by pulses of opposite sign was consistently obtained. The current-voltage (I-V) curves exhibited two transient peaks at voltages corresponding to the two steps in ΔV_FB vs. V_gate that were attributed to a displacement current from the substrate to the nanocrystal layers. Clear improvement of charge retention in the double-nanocrystal layer structure compared to the single one was obtained, opening the possibility for lowering the gate oxide thickness of the NC memory without compromising device reliability.     

Thermal and plasma enhanced atomic layer deposition ruthenium and electrical characterization as a metal electrode

Ruthenium thin films were grown by thermal and plasma-enhanced atomic layer deposition (PE-ALD) using O₂ and ammonia (NH₃) plasma, respectively. RuCp₂ and Ru(EtCp)₂ were used as Ru precursors. Pure and low resistivity (<20 μΩ cm) Ru films were grown by PE-ALD as well as thermal ALD. PE-ALD Ru showed no nucleation delay on various substrates including TaN_x, Si, and SiO₂, in contrast to thermal ALD Ru. And the root-mean-square (RMS) roughness of PE-ALD Ru was lower than that of thermal ALD Ru. Additionally, metal-oxide-semiconductor (MOS) capacitor composed of p-Si/ALD Ta₂O₅/ALD Ru (35 nm) was fabricated and C-V measurements were performed for as-deposited sample. Very small hysteresis of 20 mV was obtained, and effective work function difference to Si substrate was minimal as −0.03 V. For comparison, MOS capacitor was fabricated using sputtered Ru and large hysteresis of 0.5 V and flat band voltage (V_FB) shift to negative value were observed. This result indicates that ALD process produces more reliable, damage free Ru gate compared to sputtering process.     

Annealing effect on the metal gate effective work function modulation for the Al/TiN/SiO2/p-Si structure

In this work, the thermal annealing effect on the metal gate effective work function (EWF) modulation for the Al/TiN/SiO₂/p-Si(1 0 0) structure was investigated. Compared with the sample of TiN/SiO₂/p-Si(1 0 0) structure, for the sample additionally capped with Al the flat band voltage has a very obvious shift as large as 0.54 V to the negative direction after forming gas annealing. It is also revealed that the thermal budget can effectively influence both the EWF of the gate electrode and the thickness of the gate dielectric layer when a post annealing at 600 °C with different soak times was applied to the samples with Al cap. Material characterization indicates that the diffusion of Al and the formation of Al oxide during annealing should be responsible for all the phenomena. The interface trap density Dit calculated from the high-frequency C-V and the laser-assisted high-frequency C-V curves show that the introduction of Al does not cause reliability problem in the Al/TiN/SiO₂/p-Si structure.     

On the temperature dependence of series resistance and interface states in Al/SiO2/p-Si (MIS) Schottky diodes

The capacitance-voltage-temperature (C-V-T) and conductance-voltage-temperature (G/w-V-T) characteristics of metal-semiconductor (Al/p-Si) Schottky diodes with thermal growth interfacial layer were investigated by considering series resistance effect in the wide temperature range (80-400 K). It is found that in the presence of series resistance, the forward bias C-V plots exhibit a peak, and experimentally shows that the peak positions shift towards higher positive voltages with increasing temperature, and the peak value of the capacitance has a maximum at 80 K. The C-V and (G/w-V) characteristics confirm that the N_ss and R_s of the diode are important parameters that strongly influence the electric parameters in (Al/SiO₂/p-Si) MIS Schottky diodes. The crossing of the G/w-V curves appears as an abnormality when seen with respect to the conventional behaviour of the ideal MS or MIS Schottky diode. It is thought that the presence of a series resistance keeps this intersection hidden and unobservable in homogeneous Schottky diodes, but it appears in the case of inhomogeneous Schottky diode. In addition, the high frequency (C_m) and conductance (G_m/w) values measured under both reverse and forward bias were corrected for the effect of series resistance to obtain the real diode capacitance.     

Characterization of current-voltage (I-V) and capacitance-voltage-frequency (C-V-f) features of Al/SiO2/p-Si (MIS) Schottky diodes

The current-voltage (I-V) characteristics of metal-insulator-semiconductor Al/SiO₂/p-Si (MIS) Schottky diodes were measured at room temperature (300 K). In addition, capacitance-voltage-frequency (C-V-f) characteristics are investigated by considering the interface states (N_ss) at frequency range 100 kHz to 1 MHz. The MIS Schottky diode having interfacial insulator layer thickness of 33 Å, calculated from the measurement of the insulator capacitance in the strong accumulation region. At each frequency, the measured capacitance decreases with increasing frequency due to a continuous distribution of the interface states. From the I-V characteristics of the MIS Schottky diode, ideality factor (n) and barrier height (Φ_b) values of 1.766 and 0.786 eV, respectively, were obtained from a forward bias I-V plot. In addition, the interface states distribution profile as a function of (E_ss − E_v) was extracted from the forward bias I-V measurements by taking into account the bias dependence of the effective barrier height (Φ_e) for the Schottky diode. The diode shows non-ideal I-V behaviour with ideality factor greater than unity. This behaviour is attributed to the interfacial insulator layer, the interface states and barrier inhomogeneity of the device. As expected, the C-V curves gave a barrier height value higher than those obtained from I-V measurements. This discrepancy is due to the different nature of the I-V and C-V measurement techniques.     

On the profile of frequency and voltage dependent interface states and series resistance in (Ni/Au)/Al0.22Ga0.78N/AlN/GaN heterostructures by using current-voltage (I-V) and admittance spectroscopy methods

In order to explain the experimental effect of interface states (N_ss) and series resistance (R_s) of device on the non-ideal electrical characteristics, current-voltage (I-V), capacitance-voltage (C-V) and conductance-voltage (G/ω-V) characteristics of (Ni/Au)/Al_0.22Ga_0.78N/AlN/GaN heterostructures were investigated at room temperature. Admittance measurements (C-V and G/ω-V) were carried out in frequency and bias voltage ranges of 2 kHz-2 MHz and (−5 V)-(+5 V), respectively. The voltage dependent R_s profile was determined from the I-V data. The increasing capacitance behavior with the decreasing frequency at low frequencies is a proof of the presence of interface states at metal/semiconductor (M/S) interface. At various bias voltages, the ac electrical conductivity (σ_ac) is independent from frequencies up to 100 kHz, and above this frequency value it increases with the increasing frequency for each bias voltage. In addition, the high-frequency capacitance (C_m) and conductance (G_m/ω) values measured under forward and reverse bias were corrected to minimize the effects of series resistance. The results indicate that the interfacial polarization can more easily occur at low frequencies. The distribution of N_ss and R_s is confirmed to have significant effect on non-ideal I-V, C-V and G/ω-V characteristics of (Ni/Au)/Al_0.22Ga_0.78N/AlN/GaN heterostructures.     

A low gate leakage current and small equivalent oxide thickness MOSFET with Ti/HfO2 high-k gate dielectric

Annealing effects on electrical characteristics and reliability of MOS device with HfO₂ or Ti/HfO₂ high-k dielectric are studied in this work. For the sample with Ti/HfO₂ higher-k dielectric after a post-metallization annealing (PMA) at 600 °C, its equivalent oxide thickness value is 7.6 Å and the leakage density is about 4.5 × 10⁻² A/cm². As the PMA is above 700 °C, the electrical characteristics of MOS device would be severely degraded.     

Fabrication and characterization of p-n junctions based on ZnO and CuPc

p-n Junctions based on zinc oxide (ZnO) and copper-phthalocyanine (CuPc) were fabricated using pulsed laser deposition and thermal evaporator techniques, respectively. Current-voltage (I-V) characteristics of the ZnO-CuPc junction showed rectifying behavior. Various junction parameters such as barrier height and ideality factor were calculated using I-V data and observed to be 0.63 ± 0.02 eV and 4.0 ± 0.3, respectively. Cheung and Norde’s method were used to compare the junction parameters obtained by I-V characteristics.     

Dielectric properties in Au/SnO2/n-Si (MOS) structures irradiated under Co-γ rays

The metal-oxide-semiconductor (MOS) structures with insulator layer thickness range of 55-430 Å were stressed with a bias of 0 V during ⁶⁰Co-γ ray source irradiation with the dose rate of 2.12 kGy/h and the total dose range was 0-5×10⁵ Gy. The real part of dielectric constant ε′, dielectric loss ε″, dielectric loss tangent tanδ and the dc conductivity σ_dc were determined from against frequency, applied voltage, dose rate and thickness of insulator layer at room temperature for Au/SnO₂/n-Si (MOS) structures from C-V capacitance and G-V conductance measurements in depletion and weak inversion before and after irradiation. The dielectric properties of MOS structures have been found to be strongly influenced by the presence of dominant radiation-induced defects. The frequency, applied voltage, dose rate and thickness dependence of ε′, ε″, tanδ and σ_dc are studied in the frequency (500 Hz-10 MHz), applied voltage (−10 to 10 V), dose rate (0-500 kGy) and thickness of insulator layer (55-430 Å) range, respectively. In general, dielectric constant ε′, dielectric loss ε″ and dielectric loss tangent are found to decrease with increasing the frequency while σ_dc is increased. Experimental results shows that the interfacial polarization can be more easily occurred at the lower frequency and/or with the number of density of interface states between Si/SnO₂ interfaces, consequently, contribute to the improvement of dielectric properties of Au/SnO₂/n-Si (MOS) structures.     

Electrical characterisation of SiON/n-Si structures for MOS VLSI electronics

In the present work, we examine the properties of SiON films grown on Si substrates by CVD in order to investigate their suitability as potential materials in replacing SiO₂ in metal-oxide-semiconductor (MOS) devices. Suitable metallization created MOS devices and electrical characterisation took place in order to identify their electrical properties. Electrical measurements included current-voltage (I-V), capacitance-conductance-voltage (C-V) measurements and admittance spectroscopy (Y−ω) allowing determination of the bulk charges and the dielectric response of the films. The analysis of the data also took into account the presence of traps at the Si/SiON interface calculated by a fast conductance technique. The interface states density was of the order of 10¹² eV⁻¹ cm⁻². The dielectric constant was found to lie between 16 and 4.5 and the corresponding bulk trapped charges were found between 8 and 113 μCb cm⁻². Post deposition annealing altered these values showing an improvement of the device behaviour. A short explanation of the above is also provided.     

Au/SnO2/n-Si (MOS) structures response to radiation and frequency

Metal-insulator-semiconductor (MOS) structures with insulator layer thickness of 290 Å were irradiated using a ⁶⁰Co (γ-ray) source and relationships of electrical properties of irradiated MOS structures to process-induced surface defects have been investigated both before and after γ-irradiation. The density of surface state distribution profiles of the sample Au/SnO₂/n-Si (MOS) structures obtained from high-low frequency capacitance technique in depletion and weak inversion both before and after irradiation. The measurement capacitance and conductance are corrected for series resistance. Series resistance (Rs) of MOS structures were found both as function of voltage, frequency and radiation dose. The C(f)-V and G(f)-V curves have been found to be strongly influenced by the presence of a dominant radiation-induced defects. Results indicate interface-trap formation at high dose rates (irradiations) is reduced due to positive charge build-up in the semiconductor/insulator interfacial region (due to the trapping of holes) that reduces the flow rate of subsequent holes and protons from the bulk of the insulator to the Si/SnO₂ interface. The series resistance decreases with increasing dose rate and frequency the radiation-induced flat-band voltage shift in 1 V. Results indicate the radiation-induced threshold voltage shift (ΔV_T) strongly dependence on radiation dose rate and frequency.     

The profile of temperature and voltage dependent series resistance and the interface states in (Ni/Au)/Al0.3Ga0.7N/AlN/GaN heterostructures

The temperature dependence of capacitance-voltage (C-V) and the conductance-voltage (G/w-V) characteristics of (Ni/Au)/Al_0.3Ga_0.7N/AlN/GaN heterostructures were investigated by considering the effect of series resistance (R_s) and interface states N_ss in a wide temperature range (79-395 K). Our experimental results show that both R_s and N_ss were found to be strongly functional with temperature and bias voltage. Therefore, they affect the (C-V) and (G/w-V) characteristics. The values of capacitance give two peaks at high temperatures, and a crossing at a certain bias voltage point (∼3.5 V). The first capacitance peaks are located in the forward bias region (∼0.1 V) at a low temperature. However, from 295 K the second capacitance peaks appear and then shift towards the reverse bias region that is located at ∼−4.5 V with increasing temperature. Such behavior, as demonstrated by these anomalous peaks, can be attributed to the thermal restructuring and reordering of the interface states. The capacitance (C_m) and conductance (G/w-V) values that were measured under both reverse and forward bias were corrected for the effect of series resistance in order to obtain the real diode capacitance and conductance. The density of N_ss, depending on the temperature, was determined from the (C-V) and (G/w-V) data using the Hill-Coleman Method.     

Interfacial microstructure and electrical properties of HfAlOx thin films on compressively strained Si83Ge17 grown by RF magnetron sputtering

Interfacial microstructure and electrical properties of HfAlO_x films deposited by RF magnetron sputtering on compressively strained Si₈₃Ge₁₇/Si substrates were investigated. HfSiO_x-dominated amorphous interfacial layer (IL) embedded with crystalline HfSi_x nano-particles were revealed by high resolution transmission electron microscopy (HRTEM) and X-ray photoelectron spectroscopy depth profile study. About 280 mV-wide clockwise capacitance-voltage(C-V) hysteresis for the HfAlO_x film deposited in Ar + N₂ mixed ambient was observed. Oxygen vacancies and interfacial defects in the HfSiO_x IL, as well as trapped charges in the boundaries between the HfSi_x nano-particles and surrounded amorphous HfSiO_x may be responsible for the large C-V hysteresis.