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1.
ZrO2 thin films with a smooth surface were synthesized on silicon by atomic vapor deposition™ using Zr[OC(CH3)3]4 as precursor. The maximum growth rate (7 nm min−1) and strongest crystalline phase were obtained at 400 °C. The increase of the deposition temperature reduced the deposition rate to 0.5 nm min−1 and changed the crystalline ZrO2 phase from cubic/tetragonal to monoclinic. These films showed no enhancement of the dominating monoclinic phase by annealing. The values of the dielectric constant (up to 32) and leakage current density (down to 1.2×10−6 A cm−2 at 1×106 V cm−1) varied depending on the deposition temperature and film thickness. The midgap density of interface states was Nit=5×1011 eV−1 cm−2. The leakage current and the density of interface states were lowered by the annealing to 10−7 A cm−2 at 1×106 V cm−1 and to 1010 eV−1 cm−2, respectively. However, this also led to a decrease of the dielectric constant.  相似文献   

2.
Aluminum nitride films were deposited, at 200 °C, on silicon substrates by RF sputtering. Effects of rapid thermal annealing on these films, at temperatures ranging from 400 to 1000 °C, have been studied. Fourier transform infrared spectroscopy (FTIR) revealed that the characteristic absorption band of Al–N, around 684 cm−1, became prominent with increased annealing temperature. X-ray diffraction (XRD) patterns exhibited a better, c-axis, (0 0 2) oriented AlN films at 800 °C. Significant rise in surface roughness, from 2.1 to 3.68 nm, was observed as annealing temperatures increased. Apart from these observations, micro-cracks were observed at 1000 °C. Insulator charge density increased from 2×1011 to 7.7×1011 cm−2 at higher temperatures, whereas, the interface charge density was found minimum, 3.2×1011 eV−1cm−2, at 600 °C.  相似文献   

3.
The microwave dielectric properties of (1 − x)CaTiO3xNd(Mg1/2Ti1/2)O3 (0.1  x  1.0) ceramics prepared by the conventional solid state method have been investigated. The system forms a solid solution throughout the entire compositional range. The dielectric constant decreases from 152 to 27 as x varies from 0.1 to 1.0. In the (1 − x)CaTiO3xNd(Mg1/2Ti1/2)O3 system, the microwave dielectric properties can be effectively controlled by varying the x value. At 1400 °C, 0.1CaTiO3–0.9Nd(Mg1/2Ti1/2)O3 has a dielectric constant (εr) of 42, a Q × f value of 35 000 GHz and a temperature coefficient of resonant frequency (τf) of −10 ppm/°C. As the content of Nd(Mg1/2Ti1/2)O3 increases, the highest Q × f value of 43 000 GHz for x = 0.9 is achieved at the sintering temperature 1500 °C.  相似文献   

4.
Heteroepitaxial LaFeO3(1 1 0) thin films with a thickness of 150 nm were grown on LaAlO3(0 0 1) by reactive sputtering in an inverted cylindrical magnetron geometry. Equilibrium conductivity was measured as a function of partial pressure of oxygen at T=1000 °C, and logσ plotted vs. logP(O2) showed a minimum in conductivity for P(O2)=10−11 atm and a linear response between 10−10 and 1 atm. This linear response makes thin films of LaFeO3 a promising material for oxygen sensor applications. We have also measured the time response of the film conductivity upon an abrupt change in the partial pressure of ambient oxygen from 10−2 to 10−3 atm, which was determined at 60 s for T=700 °C and <3.5 s at T=1000 °C.  相似文献   

5.
Dependence of oxygen partial pressures on structural and electrical characteristics of HfAlO (Hf:Al=1:1) high-k gate dielectric ultra-thin films grown on the compressively strained Si83Ge17 by pulsed-laser deposition were investigated. The microstructure and the interfacial structure of the HfAlO thin films grown under different oxygen partial pressures were studied by transmission electron microscopy, and the their electrical properties were characterized by capacitance–voltage (CV) and conductance–voltage measurements. Dependence of interfacial layer thickness and CV characteristics of the HfAlO films on the growth of oxygen pressure was revealed. With an optimized oxygen partial pressure, an HfAlO film with an effective dielectric constant of 16 and a low interface state density of 2.1×1010 cm−2 eV−1 was obtained.  相似文献   

6.
This work is an attempt to estimate the electrical properties of SiO2 thin films by recording and analyzing their infrared transmission spectra. In order to study a big variety of films having different infrared and electrical properties, we studied SiO2 films prepared by low pressure chemical vapor deposition (LPCVD) from SiH4 + O2 mixtures at 425 °C and annealed at 750 °C and 950 °C for 30 min. In addition thermally grown gate quality SiO2 films of similar thickness were studied in order to compare their infrared and electrical properties with the LPCVD oxides. It was found that all studied SiO2 films have two groups of Si–O–Si bridges. The first group corresponds to bridges located in the bulk of the film and far away from the interfaces, the grain boundaries and defects and the second group corresponds to all other bridges located near the interfaces, the grain boundaries and defects. The relative population of the bulk over the boundary bridges was found equal to 0.60 for the LPCVD film after deposition and increased to 4.0 for the LPCVD films after annealing at 950 °C. Thermally grown SiO2 films at 950 °C were found to have a relative population of Si–O–Si bridges equal to 3.9. The interface trap density of the LPCVD film after deposition was found equal to 5.47 × 1012 eV−1 cm−2 and decreases to 6.50 × 1010 eV−1 cm−2 after annealing at 950 °C for 30 min. The interface trap density of the thermally grown film was found equal to 1.27 × 1011 eV−1 cm−2 showing that films with similar Si–O–Si bridge populations calculated from the FTIR analysis have similar interface trap densities.  相似文献   

7.
In this work hafnium oxide (HfO2) was deposited by r.f. magnetron sputtering at room temperature and then annealed at 200 °C in forming gas (N2+H2) and oxygen atmospheres, respectively for 2, 5 and 10 h. After 2 h annealing in forming gas an improvement in the interface properties occurs with the associated flat band voltage changing from −2.23 to −1.28 V. This means a reduction in the oxide charge density from 1.33×1012 to 7.62×1011 cm−2. After 5 h annealing only the dielectric constant improves due to densification of the film. Finally, after 10 h annealing we notice a degradation of the electrical film's properties, with the flat band voltage and fixed charge density being −2.96 V and 1.64×1012 cm−2, respectively. Besides that, the leakage current also increases due to crystallization. On the other hand, by depositing the films at 200 °C or annealing it in an oxidizing atmosphere no improvements are observed when comparing these data to the ones obtained by annealing the films in forming gas. Here the flat band voltage is more negative and the hysteresis on the CV plot is larger than the one recorded on films annealed in forming gas, meaning a degradation of the interfacial properties.  相似文献   

8.
We have fabricated thin catalytic metal–insulator–silicon carbide based structure with palladium (Pd) gates using TiO2 as the dielectric. The temperature stability of the capacitor is of critical importance for use in the fabrication of electronics for deployment in extreme environments. We have evaluated the response to temperatures in excess of 450 °C in air and observed that the characteristics are stable. Results of high temperature characterization are presented here with extraction of interface state density up to 650 °C. The results show that at temperatures below 400 °C the capacitors are stable, with a density of interface traps of approximately 6×1011 cm2 eV−1. Above this temperature the CV and GV characteristics show the influence of a second set of traps, with a density around 1×1013 cm2 eV−1, which is close to that observed for slow states near the conduction band edge. The study of breakdown field as a function of temperature shows two distinct regions, below 300 °C where the breakdown voltage has a strong temperature dependence and above 300, where it is weaker. We hypothesize that the oxide layer dominates the breakdown voltage at low temperature and the TiO2 layer above 300 °C. These results at high temperatures confirms the suitability of the Pd/TiO2/SiO2/SiC capacitor structure for stable operation in high temperature environments.  相似文献   

9.
Accelerated lifetest results are presented on HBTs with InGaP emitters. An Arrhenius plot indicates the existence of a temperature dependent activation energy, Ea. A low Ea mechanism dominates above Tj 380 °C and a high Ea mechanism dominates at lower temperature. The critical transition temperature between regimes is determined using the method of maximum likelihood. The difference in Ea’s between low and high temperature regimes is statistically significant.A comparison is made between lifetimes determined from at temperature vs. 40 °C data. No significant difference is observed indicating that beta degradation can be monitored at temperature only and cooling to low temperature is not necessary. Other comparisons indicate that junction temperatures up to 367 °C can still provide good estimates of lower temperature behavior.By the method of maximum likelihood, the predicted MTTF at Tj = 125 °C is 7.6 × 109 h with 95% CBs of [6.4 × 108, 8.9 × 1010]. Given the typical industry standard of 1 × 106 h, the reliability requirements are easily met.It is suggested that the standard of 1 × 106 h does not adequately capture failure time variation and that a better specification is in terms of fails in time (FITs). The 10 year average FIT rate at 125 °C is found to be negligible. Assuming a much higher junction temperature of 210 °C, the average failure rate climbs to 5 FITs with an upper 95% confidence bound of 40 FITs.  相似文献   

10.
In this paper, HfO2 dielectric films with blocking layers (BL) of Al2O3 were deposited on high resistivity silicon-on-insulator (HRSOI), and the interfacial and electrical properties are reported. High-resolution transmission electron microscopy (HRTEM) indicated that BL could thin the interfacial layer, keep the interface smooth, and retain HfO2 amorphous after annealing. Energy dispersive X-ray spectroscopy (EDS) and X-ray photoelectron spectroscopy (XPS) confirmed that BL weaken Si diffusion and suppressed the further growth of HfSiO. Electrical measurements indicated that there was no hysteresis was observed in capacitance–voltage curves, and Flatband shift and interface state density is 0.05 V and −1.3 × 1012 cm−2, respectively.  相似文献   

11.
Results of a study of electrically active defects induced in Sb-doped Ge crystals by implantations of hydrogen and helium ions (protons and alpha particles) with energies in the range from 500 keV to 1 MeV and doses in the range 1×1010–1×1014 cm−2 are presented in this work. Transformations of the defects upon post-implantation isochronal anneals in the temperature range 50–350 °C have also been studied. The results have been obtained by means of capacitance–voltage (CV) measurements and deep-level transient spectroscopy (DLTS).It was found from an analysis of DLTS spectra that low doses (<5×1010 cm−2) of H and He ion implantations resulted in the introduction of damage similar to that observed after MeV electron irradiation. The Sb–vacancy complex was the dominant deep-level defect in the lightly implanted samples. After implantations with doses higher than 5×1010 cm−2 peaks due to more complex defects were observed in the DLTS spectra. Implantations with heavy (5×1013 cm−2) doses of both H and He ions caused the formation of a sub-surface layer with a high (up to 1×1017 cm−3) concentration of donors. These donors were eliminated by anneals at temperatures in the range 100–200 °C. Heat treatments of the heavy proton-implanted Ge samples in the temperature range 250–300 °C resulted in the formation of shallow hydrogen-related donors, the concentration of which was the highest in a region close to the projected depth of implanted protons. The maximum peak concentration of the H-related donors was higher than 1×1015 cm−3 for a proton implantation dose of 1×1014 cm−2.  相似文献   

12.
We report measured evolutions of the optical band gap, refractive index and relative dielectric constant of TiO2 films obtained by electron beam gun evaporation and annealed in an oxygen environment. A negative shift of the flat band voltage with increasing annealing temperatures, for any film thickness, is observed. A dramatic reduction of the leakage current by about four orders of magnitude to 5×10−6 A cm−2 (at 1 MV cm−1) after 700°C and 60 min annealing is found for films thinner than 15 nm. The basic carrier transport mechanisms at different ranges of applied voltage such as hopping, space charge limited current and Fowler–Nordheim is established. An equivalent SiO2 thickness in order of 3.5 nm is demonstrated.  相似文献   

13.
Metal–insulator–metal (MIM) transparent capacitors were prepared by pulsed laser deposition (PLD) on glass substrates. The effect of the thickness of the dielectric layer and oxygen pressure on structural, electrical, and optical properties of these capacitors was investigated. Experimental results show that film thickness and oxygen pressure have no effect on the structural properties. It is also found that the optical properties of the HfO2 thin films depend strongly on both the film thickness and oxygen pressure. The electrical properties of transparent capacitors were investigated at various thickness of the dielectric layer. The capacitor shows an overall high performance, such as a high dielectric constant of 28 and a low leakage current of 2.03×10−6 A/cm2 at ±5 V. Transmittance above 70% was observed in visible region.  相似文献   

14.
Ballistic electron emission microscopy (BEEM) and ballistic electron emission spectroscopy have been performed on polycrystalline and epitaxial CoSi2/n-Si(1 0 0) contacts at temperatures ranging from −144°C to −20°C. The ultra-thin CoSi2 films (10 nm) were fabricated by solid state reaction of a single layer of Co (3 nm) or a multilayer of Ti (1 nm)/Co (3 nm)/amorphous-Si(1 nm)/Ti (1 nm) with a Si substrate, respectively. The spatial distribution of barrier height over the contact area obeys a Gaussian function at each temperature. The mean barrier height increases almost linearly with decreasing temperature with a coefficient of −0.23±0.02 meV/K for polycrystalline CoSi2/Si diodes and −0.13±0.03 meV/K for epitaxial diodes. This is approximately equal to one or one-half of the temperature coefficient of the indirect energy gap in Si, respectively. It suggests that the Fermi level is pinned to different band positions of Si. The width of the Gaussian distribution is about 30–40 meV, without clear dependence on the temperature. The results obtained from conventional current–voltage and capacitance–voltage (IV/CV) measurements are compared to BEEM results.  相似文献   

15.
The defects induced by inductively coupled plasma reactive ion etching (ICP-RIE) on a Si-doped gallium nitride (GaN:Si) surface have been analyzed. According to the capacitance analysis, the interfacial states density after the ICP-etching process may be higher than 5.4 × 1012 eV−1 cm−2, compared to around 1.5 × 1011 eV−1 cm−2 of non-ICP-treated samples. After the ICP-etching process, three kinds of interfacial states density are observed and characterized at different annealing parameters. After the annealing process, the ICP-induced defects could be reduced more than one order of magnitude in both N2 and H2 ambient. The H2 ambient shows a better behavior in removing ICP-induced defects at a temperature around 500 °C, and the interfacial states density around 2.2 × 1011 eV−1 cm−2can be achieved. At a temperature higher than 600 °C, the N2 ambient provides a much more stable interfacial states behavior than the H2 ambient.  相似文献   

16.
The trapping/detrapping behavior of charge carriers in ultrathin SiO2/TiO2 stacked gate dielectric during constant current (CCS) and voltage stressing (CVS) has been investigated. Titanium tetrakis iso-propoxides (TTIP) was used as the organometallic source for the deposition of ultra-thin TiO2 films at low temperature (<200 °C) on strained-Si/relaxed-Si0.8Ge0.2 heterolayers by plasma-enhanced chemical vapor deposition (PECVD) in a microwave (700 W, 2.45 GHz) plasma cavity discharge system at a pressure of 66.67 Pa. Stress-induced leakage current (SILC) through SiO2/TiO2 stacked gate dielectric is modeled by taking into account the inelastic trap-assisted tunneling (ITAT) mechanism via traps located below the conduction band of TiO2 layer. The increase in the gate current density observed during CVS from room temperature up to 125 oC has been analyzed and modeled considering both the buildup of charges in the layer as well as the SILC contribution. Trap generation rate and trap cross-section are extracted. A capture cross-section in the range of 10−19 cm2 as compared to 10−16 cm2 in SiO2 has been observed. A temperature-dependent trap generation rate and defects have also been investigated using time-dependent current density variation during CVS. The time dependence of defect density variation is calculated within the dispersive transport model, assuming that these defects are produced during random hopping transport of positively charge species in the insulating high-k stacked layers. SILC generation kinetics, i.e. defect generation probability under different injected fluences for various high-constant stress voltages in both polarities have been studied. An empirical relation between trap generation probability and applied stress voltage for various injected fluences has been developed.  相似文献   

17.
The growth of Pr2O3 layers on Si(1 1 1) has been studied by X-ray diffraction, Low-energy electron diffraction (LEED) and atomic force microscopy (AFM). Pr2O3 starts to grow as a 0.6-nm thick layer corresponding to one unit cell of the hexagonal phase (1 ML). The X-ray results indicate that layers thicker than 0.6 nm do not grow with the hexagonal phase. Growth takes place at a sample temperature of 500–550 °C. Annealing of the monolayer in UHV at a temperature above 700 °C leads to the formation of Pr2O3 and PrSi2 islands. Silicide islands are found only at annealing in UHV and do not occur at annealing in oxygen atmosphere of 10−8 mbar. The LEED pattern after heating to 730 °C shows a (2×2) and (√3×√3) superstructure and after heating to 1000 °C a (1×5) superstructure occurs. The superstructures seen in the LEED pattern arise from silicide structures in the area between the islands. The silicide remains on the surface and cannot be removed with flashing to 1100 °C. Further deposition of Pr2O3 on the surface covered with silicide phases does not lead to growth of ordered layers.  相似文献   

18.
SrTiO3 thin films (STO), were deposited on Si(100) covered by 2 nm of SiO2, at different temperatures from 450 °C to 850 °C using liquid injection MOCVD, the bimetallic precursor being Sr2Ti2(OiPr)8(tmhd)4. The STO films were analysed by XRD, FTIR, SIMS and TEM. An amorphous layer was observed between STO and SiO2/Si. The nature and thickness of the interlayer were determined, as well as the most favourable conditions for a good quality crystalline STO film, and a reduced interlayer.  相似文献   

19.
This paper describes realization and characterization of SrTiO3 (STO) high K MIM capacitors above BiCMOS integrated circuit (IC). These capacitances are connected to IC and are used as coupling capacitors in order to realize a high pass filter. Surface capacitance achieved is 10 nF/mm2 with capacitance value of 1.2 nF. The process for STO MIM fabrication does not exceed 400 °C, which is compatible with interconnections. Typical K and dielectric losses values obtained are, respectively 110% and 2%. Yield obtained reaches 83% for capacitors. A functional high pass filter using these STO capacitors was realized in this study. It exhibits a cut-off frequency at 6.5 kHz and a constant gain at higher frequencies of −1.3 dB.  相似文献   

20.
Using hydrofluoric acid (HF) as catalyst, nanoporous SiO2 thin film was synthesized by sol–gel method. By scanning electron microscopy, Fourier transform infrared spectra, thermo gravimetric and differential thermal analysis, ellipsometry, capacitance–voltage and current–voltage measurements, the effects of annealing on film properties were discussed in detail. The introduction of HF results in the less polarizability, the preferable microstructures and the improved thermal stability of the nanoporous silica films. After thermal annealing at 450 °C, the crack-free films with strong hydrophobicity, ultra-low dielectric constant of 1.65, porosity of 78%, and leakage current density of 1.3 × 10−8 A cm−2 were obtained.  相似文献   

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