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1.
In this investigation, we have fabricated Ta(Vb)/Si(111) and Cu/Ta(Vb)/Si(111) systems using a DC bias sputtering technique at high Ar pressure (100 mTorr). For Ta/Si(111) system, tantalum layer was formed under various bias voltages ranging from 0 to −150 V. The films were characterized by Rutherford backscattering spectrometry (RBS), scanning electron microscopy (SEM) and four-point probe sheet resistance measurements (Rs). From electrical resistivity and SEM data, a minimum resistivity (99 μΩ cm) and well surface morphology at an optimum bias voltage (Vb=−50 V) was obtained for the Ta(Vb)/Si(111) system. The Ta films deposited under these conditions with 50 nm thickness are then used as a diffusion barrier in the Cu/Ta(Vb)/Si(111) multilayer structure. According to our RBS, SEM and Rs analysis, the Ta barrier layer formed under the controlled bias sputtering at high Ar pressure has demonstrated an improved Ta structure with excellent thermal stability up to 650°C for the Cu/Ta(Vb)/Si(111) system annealed in N2 environment for 30 min. Formation of TaSi2 was observed at 700°C after the barrier failure using RBS spectra.  相似文献   

2.
Cobalt-coated single-crystal Si-Ge layers grown epitaxially by ultrahigh vacuum chemical vapor deposition on silicon substrates were annealed by rapid thermal annealing in the temperature range from 450 °C to 800 °C for periods ranging from 1 to 3 min. The measured sheet resistivities of the films exhibit strong dependence on the annealing conditions. The Co-SiGe film annealed at 700 °C for 3 min had the lowest sheet resistivity (3Ω/p). Structural studies using cross-sectional transmission electron microscopy showed that the cobalt films reacted with the SiGe layer and the thickness of the resulting film increases with increasing annealing temperature or time. Electron diffraction and X-ray microanalysis using energy-dispersive spectrometry showed that CoSi2 was formed during initial annealing. The detection of germanium in the reacted layer and the deviation of the reacted layer's lattice constant from that of CoSi2 indicated that germanium diffused into the CoSi2 and formed ternary compounds (CoxSiyGez) during further annealing.  相似文献   

3.
Pt-PtOx thin films were prepared on Si(100) substrates at temperatures from 30 to 700°C by reactive r.f. magnetron sputtering with platinum target. Deposition atmosphere was varied with O2/Ar flow ratio. The deposited films were characterized by X-ray diffraction, X-ray photoelectron spectroscopy and scanning electron microscopy. Resistively of the deposited films was measured by d.c. four probe method. The films mainly consisted of amorphous PtO and Pt3O4 (or Pt2O3) below 400°C, and amorphous Pt was increased in the film as a deposition temperature increased to 600°C. When deposition temperature was thoroughly increased, (111) oriented pure Pt films were formed at 700°C. Compounds included in the films strongly depended on substrate temperature rather than O2/Ar flow ratio. Electrical resistivity of Pt-PtOx films was measured to be from the order of 10−1 Ω cm to 10−5 Ω cm, which was related to the amount of Pt phase included in the deposited films.  相似文献   

4.
The BaxSr1−xTiO3 (BST)/Pb1−xLaxTiO3 (PLT) composite thick films (20 μm) with 12 mol% amount of xPbO–(1 − x)B2O3 glass additives (x = 0.2, 0.35, 0.5, 0.65 and 0.8) have been prepared by screen-printing the paste onto the alumina substrates with silver bottom electrode. X-ray diffraction (XRD), scanning electron microscope (SEM) and an impedance analyzer and an electrometer were used to analyze the phase structures, morphologies and dielectric and pyroelectric properties of the composite thick films, respectively. The wetting and infiltration of the liquid phase on the particles results in the densification of the composite thick films sintered at 750 °C. Nice porous structure formed in the composite thick films with xPbO–(1 − x)B2O3 glass as the PbO content (x) is 0.5 ≥ x ≥ 0.35, while dense structure formed in these thick films as the PbO content (x) is 0.8 ≥ x ≥ 0.65. The volatilization of the PbO in PLT and the interdiffusion between the PLT and the glass lead to the reduction of the c-axis of the PLT phase. The operating temperature range of our composite thick films is 0–200 °C. At room temperature (20 °C), the BST/PLT composite thick films with 0.35PbO–0.65B2O3 glass additives provided low heat capacity and good pyroelectric figure-of-merit because of their porous structure. The pyroelectric coefficient and figure-of-merit FD are 364 μC/(m2 K) and 14.3 μPa−1/2, respectively. These good pyroelectric properties as well as being able to produce low-cost devices make this kind of thick films a promising candidate for high-performance pyroelectric applications.  相似文献   

5.
Solid solutions of Bi3(Nb1−xTax)O7 (x = 0.0, 0.3, 0.7, 1) were synthesized using solid state reaction method and their microwave dielectric properties were first reported. Pure phase of fluorite-type could be obtained after calcined at 700 °C (2 h)−1 between 0 ≤ x ≤ 1 and Bi3(Nb1−xTax)O7 ceramics could be well densified below 990 °C. As x increased from 0.0 to 1.0, saturated density of Bi3(Nb1−xTax)O7 ceramics increased from 8.2 to 9.1 g cm−3, microwave permittivity decreased from 95 to 65 while Qf values increasing from 230 to 560 GHz. Substitution of Ta for Nb modified temperature coefficient of resonant frequency τf from −113 ppm °C−1 of Bi3NbO7 to −70 ppm °C−1 of Bi3TaO7. Microwave permittivity, Qf values and τf values were found to correlate strongly with the structure parameters of fluorite solid solutions and the correlation between them was discussed in detail. Considering the low densified temperature and good microwave dielectric proprieties, solid solutions of Bi3(Nb1−xTax)O7 ceramics could be a good candidate for low temperature co-fired ceramics application.  相似文献   

6.
AgInSnxS2−x (x = 0–0.2) polycrystalline thin films were prepared by the spray pyrolysis technique. The samples were deposited on glass substrates at temperatures of 375 and 400 °C from alcoholic solutions comprising silver acetate, indium chloride, thiourea and tin chloride. All deposited films crystallized in the chalcopyrite structure of AgInS2. A p-type conductivity was detected in the Sn-doped samples deposited at 375 °C, otherwise they are n-type. The optical properties of AgInSnxS2−x (x < 0.2) resemble those of chalcopyrite AgInS2. Low-temperature PL measurements revealed that Sn occupying an S-site could be the responsible defect for the p-type conductivity observed in AgInSnxS2−x (x < 2) thin films.  相似文献   

7.
In this paper, bulk-Si metal–oxide–semiconductor field effect transistors (MOSFETs) are fabricated using the catalytic chemical vapor deposition (Cat-CVD) method as an alternative technology to the conventional high-temperature thermal chemical vapor deposition. Particularly, formation of low-resistivity phosphorus (P)-doped poly-Si films is attempted by using Cat-CVD-deposited amorphous silicon (a-Si) films and successive rapid thermal annealing (RTA) of them. Even after RTA processes, neither peeling nor bubbling are observed, since hydrogen contents in Cat-CVD a-Si films can be as low as 1.1%. Both the crystallization and low resistivity of 0.004 Ω·cm are realized by RTA at 1000 °C for only 5 s. It is also revealed that Cat-CVD SiNx films prepared at 250 °C show excellent oxidation resistance, when the thickness of films is larger than approximately 10 nm for wet O2 oxidation at 1100 °C. It is found that the thickness required to stop oxygen penetration is equivalent to that for thermal CVD SiNx prepared at 750 °C. Finally, complementary MOSFETs (CMOSs) of single-crystalline Si were fabricated by using Cat-CVD poly-Si for gate electrodes and SiNx films for masks of local oxidation of silicon (LOCOS). At 3.3 V operation, less than 1.0 pA μm−1 of OFF leakage current and ON/OFF ratio of 107–108 are realized, i.e. the devices can operate similarly to conventional thermal CVD process.  相似文献   

8.
We succeeded in obtaining strained Si1−yCy films at a substrate temperature of 200 °C by the hot-wire cell method. The substitutional carbon concentration in films annealed at 700 °C was 0.9%, while it was limited to 0.13% for a sample grown by gas-source molecular beam epitaxy (MBE) at a substrate temperature of 700 °C. We investigated the thermal stability of strained Si1−yCy films for device application. Annealing at over 900 °C caused the formation of 3C-SiC and relaxation of the strain occurred. From this result, we found that the process temperature should be lower than 800 °C. A low-temperature MOSFET process, in which all process temperatures after deposition of Si1−yCy were lower than 800 °C, was developed and a strained Si1−yCy MOSFET was fabricated.  相似文献   

9.
High quality and thin relaxed SiGe films were grown on Si (0 0 1) using ultra high vacuum chemical vapor deposition (UHV/CVD) by employing an intermediate Si1−yCy layer. The Si1−yCy/SiGe bilayer was found to change mechanism of relaxation in the SiGe overlayer. Compared with the samples with a Si layer, the equilibrium critical thickness of top SiGe films with rough surface by introducing an intermediate Si0.986C0.014 layer are drastically reduced; this result was attributed to larger tensile stress in the inserted Si0.986C0.014 layer. With a 210-nm-thick Si0.8Ge0.2 overlayer, this Si0.8Ge0.2/Si0.986C0.014/Si0.8Ge0.2 heterostructure has a threading dislocation density (TDs) less than 1 × 105 cm−2 and a residual strain of 30%. The root mean square (RMS) of surface roughness for this sample was measured to be about 1.8 nm. In this SiGe/Si1−yCy/SiGe structure, C atoms in the intermediate Si layer will improve the relaxation of thin SiGe overlayer, however, the relaxation for the 700-nm-thick SiGe overlayer is independent of the addition of C. The point defects rich Si0.986C0.014 layer plays the role to confine the misfit dislocations, which formed at the interface of the top Si0.8Ge0.2 and the Si0.986C0.014 layer, and blocked the propagation of TDs. Strained-Si n-channel metal-oxide-semiconductor transistors (n-MOSFETs) with a 210-nm-thick Si0.8Ge0.2 overlayers as buffer were fabricated and examined. Drain current and effective electron mobility for the strained-Si device with this novel substrate technology was found to be 100 and 63% higher than that of control Si device. Our results show that thin relaxed Si0.8Ge0.2 films with the intermediate Si0.986C0.014 layer serve as good candidates for high-speed strained-Si devices.  相似文献   

10.
Chang Jung Kim   《Thin solid films》2004,450(2):261-264
Ferroelectric bismuth lanthanum titanate (Bi3.25La0.75Ti3O12; BLT) thin films were deposited on Pt/TiO2/SiO2/Si substrate by chemical solution deposition method. The films were crystallized in the temperature range of 600–700 °C. The spontaneous polarization (Ps) and the switching polarization (2Pr) of BLT film annealed at 700 °C for 30 min were 22.6 μC/cm2 and 29.1 μC/cm2, respectively. Moreover, the BLT capacitor did not show any significant reduction of hysteresis for 90 min at 300 °C in the forming gas atmosphere.  相似文献   

11.
Nanocrystalline Ba1−xSrxTiO3 (x=0, 0.2, 0.4, 0.6, 0.8 and 1.0) precursors were synthesized using the stearic acid gel method. After the precursors had been calcined at 600–950°C for 0.5–1 h, nanocrystalline powders with the cubic perovskite structure were obtained and these were made into thick films. The powder samples were characterized by differential thermal analysis, X-ray diffraction and transmission electron microscopy, and the thick film samples were characterized by scanning electron microscopy and X-ray diffraction. The humidity-sensitive properties of the nanocrystalline Ba1−xSrxTiO3 thick films were investigated. The results show that these nanocrystalline thick films possess higher humidity sensitivity and lower resistance than those of conventional materials.  相似文献   

12.
Thermoelectric bismuth telluride thin films were prepared on SiO2/Si substrates by radio-frequency (RF) magnetron sputtering. Co-sputtering method with Bi and Te targets was adopted to control films' composition. BixTey thin films were elaborated at various deposition temperatures with fixed RF powers, which yielded the stoichiometric Bi2Te3 film deposition without intentional substrate heating. The effects of deposition temperature on surface morphology, crystallinity and electrical transport properties were investigated. Hexagonal crystallites were clearly visible at the surface of films deposited above 290 °C. Change of dominant phase from rhombohedral Bi2Te3 to hexagonal BiTe was confirmed with X-ray diffraction analyses. Seebeck coefficients of all samples have negative value, indicating the prepared BixTey films are n-type conduction. Optimum of Seebeck coefficient and power factor were obtained at the deposition temperature of 225 °C (about − 55 μV/K and 3 × 10− 4 W/K2·m, respectively). Deterioration of thermoelectric properties at higher temperature could be explained with Te deficiency and resultant BiTe phase evolution due to the evaporation of Te elements from the film surface.  相似文献   

13.
(Ti, Al)N films have drawn much attention as alternatives for TiN coatings, which are oxidized easily in air above 500 °C. We have investigated the effect of Al content on the oxidation resistance of (Ti1 − xAlx)N films prepared by r.f. reactive sputtering.

(Ti1 − xAlxN films (O ≤ x ≤ 0.55) were deposited onto fused quartz substrates by r.f. reactive sputtering. Composite targets with five kinds of Al-to-Ti area ratio were used. The sputtering gas was Ar (purity, 5 N) and N2 (5 N). The flow rate of Ar and N2 gas was kept constant at 0.8 and 1.2 sccm, respectively, resulting in a sputtering pressure of 0.4 Pa. The r.f. power was 300 W for all experiments. Substrates were not intentionally heated during deposition. The deposited films (thickness, 300 nm) were annealed in air at 600 900 °C and then subjected to X-ray diffractometer and Auger depth profiling.

The as-deposited (Ti1 − xAlx)N films had the same crystal structure as TiN (NaCl type). Al atoms seemed to substitute for Ti in lattice sites. The preferential orientation of the films changed with the Al content of the film, x. Oxide layers of the films grew during annealing and became thicker as the annealing temperature increased. The thickness of the oxide layer grown on the film surface decreased with increasing Al content in the film. For high Al content films an Al-rich oxide layer was grown on the surface, which seemed to prevent further oxidation. All of the films, however, were oxidized by 900 °C annealing, even if the Al content was increased up to 0.55.  相似文献   


14.
Highly preferred oriented lead barium titanate (Pb1−x,Bax)TiO3 thin film, with particular emphasis on (Pb0.5,Ba0.5)TiO3, can be obtained by spin-coating on MgO (100) substrate by using the precursor sol, which was synthesized from acetylacetone chelating with titanium isopropoxide and ethylene glycol as a solvent, in the sol-gel process. Film thickness, pyrolysis temperature and heating rate were studied systemically to investigate their influences on the formation of preferred oriented thin films. The highly preferred (001)/(100) oriented thin film could be obtained by the pyrolysis of wet film at 500 °C and annealing at 600 °C at a slow heating rate of 5 °C/min. It is confirmed that the tetragonal perovskite structure of the titanate ceramic decreases with an increase of Ba content in (Pb1−x,Bax)TiO3. The (001)/(100) oriented films were synthesized from all compositions between x = 0.2 and x = 0.8, at a crystallization temperature of 600 °C. In particular, for the Ba content in the range of x = 0.50.6, highly preferred (001)/(100) planes were observed.  相似文献   

15.
G. V Gadiyak   《Thin solid films》1999,350(1-2):147-152
A simple model of thermal dissociation and recovery of hydrogen-passivated silicon defects at the Si/SiO2 interface, such as Pb - centers, during vacuum thermal annealing has been suggested. his model considers reactions of hydrogen with defect states at the Si/SiO2 interface and diffusion of liberated atomic and molecular hydrogen in a silicon dioxide film. The rate constants were calculated in diffusion approximation. A good agreement was obtained between the experimental and numerical simulation results for oxides with different thickness (204–1024 Å), grown, both, (111) and (100) samples and annealed in the temperature range (480–700°C).  相似文献   

16.
Bian Bo  Yie Jian  Cao Yi  Wu Zi-Qin   《Thin solid films》1993,230(2):160-166
The crystallization behavior of a-Si1−xCx:H/Al films after annealing has been investigated by transmission electron microscopy and Raman scattering. It is found that the crystallization process is complex and non-uniform, and that both equiaxial and branching Si grains with many twins and stacking faults arise at annealing temperatures as low as 250 °C. Both fine polycrystalline β-SiC grains and fractal-like -SiC aggregates are first observed in a few regions in a-Si1−xCx:H/Al films annealed at 350 °C. The increase of the Al grain size can cause a decrease in the crystallization temperature and a rise in the grain growth rate of Si. At higher annealing temperatures, the reaction process SiC+Al→Al4C3+Si is predominant.  相似文献   

17.
Metal-organic chemical vapour deposition (MOCVD) of various phases in PrOx system has been studied in relation with deposition temperature (450–750 °C) and oxygen partial pressure (0.027–100 Pa or 0.2–750 mTorr). Depositions were carried out by pulsed liquid injection MOCVD using Pr(thd)3 (thd = 2,2,6,6-tetramethyl-3,5-heptanedionate) precursor dissolved in toluene or monoglyme. By varying deposition temperature and oxygen partial pressure amorphous films or various crystalline PrOx phases (Pr2O3, Pr7O12, Pr6O11) and their mixtures can be grown. The pure crystalline Pr2O3 phase grows only in a narrow range of partial oxygen pressure and temperature, while high oxygen pressure (40–100 Pa) always leads to the most stable Pr6O11 phase. The influence of annealing under vacuum at 750 °C on film phase composition was also studied. Near 90% step coverage conformity was achieved for PrOx films on structured silicon substrates with aspect ratio 1:10. In air degradation of Pr2O3 films with transformation to Pr(OH)3 was observed in contrast to Pr6O11 films.  相似文献   

18.
Tantalum oxide films have been deposited by 355 nm pulsed laser ablation of metallic Ta target in O3/O2 ambient. The structure and the composition of as-deposited and annealed films were examined by X-ray diffraction and Fourier transform infrared spectroscopy. The measurements of the current–voltage and capacitance–voltage characteristics of the Al/Ta2O5/Si capacitors were performed to reveal the electrical properties of the Ta2O5 films. The effects of annealing temperature on the characteristics of thin films have been studied. The results suggest that the films annealed above 700°C have the structure of orthorhombic β-Ta2O5, thc annealing treatment at high temperature decreases the bulk trap charge, the border trap, and the interface trap densities of as-deposited films, and improves significantly the dielectric and electrical properties of Ta2O5 film.  相似文献   

19.
Electroplated Cu film on a thin seed layer of IMP deposited Cu has been investigated in the EPCu (1 m)/IMPCu (150 nm)/TaN (25 nm)/SiO2(500 nm)/Si multi-layer structure. The characteristics of Electroplated-Cu films before and after annealing were investigated by means of sheet resistance, X-ray diffraction (XRD), Scanning Electron Microscopy (SEM), and Rutherford Backscattering Spectroscopy (RBS). Annealing at temperatures of higher than 750°C resulted in slightly higher sheet resistance, larger grain sizes and rougher surface. SEM micrograph showed that the agglomeration of EP-Cu film occurred only at annealing temperatures higher than 850°C. During annealing, the EP-Cu grain grew normally and their sizes increased to about five times larger than the thickness of the EP-Cu film but the (111) preferred orientation was maintained up to 950°C. Furthermore, the interfacial reactions between Cu layer and IMP-TaN diffusion barrier were also detected at annealing temperatures of higher than 750°C.  相似文献   

20.
CaCu3Ti4O12 (CCTO) thin films were successfully deposited on Pt/Ti/SiO2/Si(1 0 0) substrates using pulsed-laser deposition technique. The crystalline structure and the surface morphology of the CCTO thin films were greatly affected by the substrate temperature and oxygen pressure. Thin films with a (2 2 0) preferential orientation were obtained at the substrate temperature above 700 °C and oxygen pressure above 13.3 Pa. The 480-nm thin films deposited under 720 °C and 26.6 Pa have a fairly high dielectric constant of near 2000 at 10 kHz and room temperature. The values of the dielectric constant and loss and their temperature-dependence under different frequency are comparable with those obtained in the epitaxial CCTO films grown on oxide substrates.  相似文献   

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