首页 | 本学科首页   官方微博 | 高级检索  
相似文献
 共查询到20条相似文献,搜索用时 31 毫秒
1.
Ferroelectric SrBi2Ta2O9/SrBi2Nb2O9 (SBT/SBN) multilayer thin films with various stacking periodicity were deposited on Pt/TiO2/SiO2/Si substrate by pulsed laser deposition technique. The X-ray diffraction patterns indicated that the perovskite phase was fully formed with polycrystalline structure in all the films. The Raman spectra showed the frequency of the O–Ta–O stretching mode for multilayer and single layer SrBi2(Ta0.5Nb0.5)2O9 (SBNT) samples was 827–829 cm−1, which was in between the stretching mode frequency in SBT (813 cm−1) and SBN (834 cm−1) thin films. The dielectric constant was increased from 300 (SBT) to 373 at 100 kHz in the double layer SBT/SBN sample with thickness of each layer being 200 nm. The remanent polarization (2Pr) for this film was obtained 41.7 μC/cm2, which is much higher, compared to pure SBT film (19.2 μC/cm2). The coercive field of this double layer film (67 kV/cm) was found to be lower than SBN film (98 kV/cm).  相似文献   

2.
We have measured Raman spectra of fluorine-doped SiO2 (SiOF) films and quartz glass. From a comparison between Raman spectra of the SiO2 film and quartz glass, it has been found that the SiO2 film is under compressive stress and that it has more threefold ring defects than quartz glass. Raman bands from threefold and fourfold ring defects in SiOF films become week as the fluorine/oxygen (F/O) ratio increases and as the stress decreases. The decrease of intensities of these Raman bands shows that ring defects in SiOF films decrease as the F/O ratio increases and as the stress decreases. The triply degenerated ω4 mode at 460 cm−1 becomes sharp as the F/O ratio increases and as the stress decreases. Furthermore, the peak-frequency of ω1 mode around 820 cm−1 decreases with a decrease of stresses whereas that of ω3 mode around 1065 cm−1 increases. These results can be well understood in terms of a decrease of O-Si-O bonding angle caused by relaxation of stresses.  相似文献   

3.
Catalytic chemical vapor deposition (Cat-CVD) has been developed to deposit alumina (Al2O3) thin films on silicon (Si) crystals using N2 bubbled tri-methyl aluminum [Al(CH3)3, TMA] and molecular oxygen (O2) as source species and tungsten wires as a catalyzer. The catalyzer dissociated TMA at approximately 600 °C. The maximum deposition rate was 18 nm min−1 at a catalyzer temperature of 1000 °C and substrate temperature of 800 °C. Metal oxide semiconductor (MOS) diodes were fabricated using gates composed of 32.5-nm-thick alumina film deposited at a substrate temperature of 400 °C. The capacitance measurements resulted in a relative dielectric constant of 7.4, fixed charge density of 1.74×1012 cm−2, small hysteresis voltage of 0.12 V, and very few interface trapping charges. The leakage current was 5.01×10−7 A cm−2 at a gate bias of 1 V.  相似文献   

4.
Bismuth titanate (Bi4Ti3O12) thin films with a high c-axis orientation up to 99% were prepared on (100)-oriented silicon wafers by r.f. planar magnetron sputtering using a Bi2TiO5 ceramic target at a substrate temperature of 600 °C. From the Auger electron spectroscopy depth profile of the film, there is no evidence of interdiffusion of a specific element between the film and the substrate. Relative dielectric constant of these films depends on film thickness. The behavior was explained assuming a low-dielectric-constant interface layer. Using this assumption, the relative dielectric constant of Bi4Ti3O12 film was estimated to be approximately 140. This value is close to that along the c axis in a bulk form. The remanent polarization and the coercive field were 0.8 μC cm−2 and 20 kV cm−1, respectively.  相似文献   

5.
In this work, high concentration erbium doping in silicon-rich SiO2 thin films is demonstrated. Si plus Er dual-implanted thermal SiO2 thin films on Si substrates have been fabricated by using a new method, the metal vapor vacuum arc ion source implantation with relatively low ion energy, strong flux and very high dose. X-Ray photoelectron spectroscopy measurement shows that very high Er concentrations on the surfaces of the samples, corresponding to 10 at.% or the doping level of 1021 atoms cm−3, are achieved. This value is much higher than that obtained by using other fabrication methods such as the high-energy ion implantation and molecular beam epitaxy. Reflective high-energy electron diffraction, atomic force microscopy and cross-section high-resolution transmission electron microscopy observations show that the excess Si atoms in SiO2 matrix accumulate to form Si clusters and then crystallize gradually into Si nanoparticles embedded in SiO2 films during dual-ion implantation followed by rapid thermal annealing. Er segregation and precipitates are not formed. Photoluminescence at the wavelength of 1.54 μm exhibits very weak temperature dependence due to the introduction of Si nanocrystals into the SiO2 matrix. The 1.54-μm light emission signals from annealed samples decrease by less than a factor of 2 when the measuring temperature increases from 77 K to room temperature.  相似文献   

6.
The optical absorption (hν) and Raman and Infra Red (IR) spectra of Si doped GaN layers deposited on sapphire through buffer layers have been recorded for electron concentrations from 5×1017 to 5×1019 cm−3. The (hν) values deduced from photothermal deflection spectroscopy (0.5–3.5 eV) and IR absorption (0.15–0.5 eV) vary between 50 and 104 cm−1 showing doping dependant free electron absorption at low energy, doping independant band gap at high energy, and slowly doping dependant defect absorption in the medium energy range. In our micro Raman geometry, maxima appear or can be deduced near the frequency expected for either the A1(LO) or the A1(LO+) modes split from the A1(LO) mode by plasmon phonon interaction. There is a large systematic evolution in the expected way for the IR reflectivity.  相似文献   

7.
In this paper we report on surface nitridation of SiO2 and on photoresist removal by using species decomposed from NH3 or H2 and generated by a heated tungsten catalyzer. The top surface of SiO2/Si(100) is nitrided at temperatures as low as 300 °C using species decomposed from NH3 species. The removal of heavy-doped, as high as 1×1016 cm−2, ion-implanted photoresist is realized using atomic hydrogen.  相似文献   

8.
P.C. Joshi  S.B. Desu 《Thin solid films》1997,300(1-2):289-294
Polycrystalline BaTiO3 thin films having the perovskite structure were successfully produced on platinum coated silicon, bare silicon, and fused quartz substrate by the combination of the metallo-organic solution deposition technique and post-deposition rapid thermal annealing treatment. The films exhibited good structural, electrical, and optical properties. The electrical measurements were conducted on metal-ferroelectric-metal (MFM) and metal-ferroelectric-semiconductor (MFS) capacitors. The typical measured small signal dielectric constant and dissipation factor at a frequency of 100 kHz were 255 and 0.025, respectively, and the remanent polarization and coercive field were 2.2 μC cm−2 and 25 kV cm−1, respectively. The resistivity was found to be in the range 1010–1012 Ω·cm, up to an applied electric field of 100 kV cm−1, for films annealed in the temperature range 550–700 °C. The films deposited on bare silicon substrates exhibited good film/substrate interface characteristics. The films deposited on fused quartz were highly transparent. An optical band gap of 3.5 eV and a refractive index of 2.05 (measured at 550 nm) was obtained for polycrystalline BaTiO3 thin film on fused quartz substrate. The optical dispersion behavior of BaTiO3 thin films was found to fit the Sellmeir dispersion formula well.  相似文献   

9.
Aerosol-gel process has been used for the deposition of SiO2 thin films. Layers were deposited from a solution with pH = 3.5 and water to TEOS molar ratio (rw) 2.2 and then treated at various temperatures ranging from room temperature to 700°C. As-prepared thin films have been characterized by FTIR spectroscopy. Spectra were acquired in transmission at 65° angle of incidence or at perpendicular incidence. Characteristic absorption bands of the SiO2 sol-gel system have been studied with respect to the posttreatment temperature. Bands located at 1250–1000 cm−1 and around 960 cm−1 have been deconvoluted in several peaks. The origin and temperature dependence of these peaks are discussed.  相似文献   

10.
Current vs. time (It) measurements were performed on Ta2O5-based devices. Charge build-up at the Ta2O5/SiO2 interface was used to explain the transient. The interfacial charge density was calculated from the It curve and the maximum was found to be 398 nC cm-2 and 317 nC cm-2 for Al/Ta2O5/Si and Al/Ta2O5/SiO2/Si capacitors respectively. The value for MTOS was comparable with the value obtained by quasi-static measurements.  相似文献   

11.
Chromium disilicide (CrSi2) films 1 000 Å thick have been prepared by molecular beam epitaxy on CrSi2 templates grown on Si(111) substrate. The effect of the substrate temperature on the structural, electrical and optical properties of CrSi2 films has been studied by transmission and scanning electron microscopies, optical microscopy, electrical resistivity and Hall effect measurements and infrared optical spectrometry. The optimal temperature for the formation of the epitaxial A-type CrSi2 film have been found to be about 750°C. The electrical measurement have shown that the epitaxial A-type CrSi2 film is p-type semiconductor having a hole concentration of 1 × 1017cm−3 and Hall mobility of 2 980 cm2 V−1 s−1 at room temperature. Optical absorption coefficient data have indicated a minimum, direct energy gap of 0.34 eV. The temperature dependence of the Hall mobility (μ) in the temperature range of T = 180–500 K can be expressed as μ = 7.8 × 1010T−3cm2V−1s−1.  相似文献   

12.
The production of highly Cu+-doped KCl films and the properties of their 266 nm absorption band, which has an off-center property in doped single crystals, open the possibility of application of these films as ultra-violet optical filters. The investigated films, of approximately 1 μm thickness, were prepared by resistive co-evaporation of KCl and CuCl powders on different substrates of CaF2, Al2O3, SiO2, KCl and Si. The Cu+ concentration, as determined by energy-dispersive X-ray, ranges from 1020 to 1021 cm−3, for 1–15% CuCl nominal mole percent concentration. Structural and optical properties were investigated through scanning electron microscopy, X-ray diffraction, ellipsometry, optical absorption and transmission. The films are polycrystalline, and the gain size decreases with increasing Cu+ impurity concentration, yielding an increase of visible transmission to a limited CuCl concentration. These films show a 6.295 Å lattice parameter with a f.c.c. structure and an index of refraction of 1.53 at 266 nm. When the Cu+ concentration is increased, the UV band position remains the same and no clusters are evidenced even to the high 15% CuCl concentration investigated, which differs very much from single crystals samples grown by the Kyropoulos-Czochralski method. For a Cu+ concentration of 8×1020 cm−3 the film shows a transmission better than 88% at 350 nm wavelength.  相似文献   

13.
Silicon oxide films have been deposited with remote plasma chemical vapour deposition (RPCVD) at low temperatures (<300 °C) from SiH4---N2O. The effect of a gas-phase reaction on the SiO2 film properties and Si/SiO2 interface was investigated. As the partial pressure ratio was increased above N2O/SiH4 = 4, a gas-phase reaction with powder formation was observed, which degraded film properties, increased surface roughness, and decreased deposition rate. When N2O/SiH4 <4, there was no detectable IR absorption in the film associated with hydrogen-related bonds (Si---OH and Si---H) but when N2O/SiH4 >4, the incorporation of Si---OH bond became significant and Si1+, intermediate state silicon at the interface, was more abundant. The oxide fixed charge, interface trap density, surface roughness and leakage current were increased when there was powder formation in the gas phase. High plasma power also favoured the powder formation in the gas phase. C---V and I---V characteristics were measured and it was shown that these electrical properties were directly related to the process condition and material properties of the oxide and the Si/SiO2 interface.  相似文献   

14.
Sejoon Lee  Yoon Shon  Deuk Young Kim   《Thin solid films》2008,516(15):4889-4893
The temperature-dependent photoluminescence (PL) properties of the As-doped (Zn0.93Mn0.07)O layer, which showed the stable p-type conductivity with carrier concentration of  1018 cm− 3 and carrier mobility of  10 cm2 V− 1 s− 1, were investigated. From fitting of the Bose–Einstein approximation using extracted emission parameters from temperature-dependent PL spectra, it was found that the interaction between exciton and phonon in p-(Zn0.93Mn0.07)O:As is higher than that in host material ZnO. This result was confirmed as resulting from the increase of disorder-activated phonon scattering which is attributed to the increase of free carriers donated from implanted As dopants.  相似文献   

15.
Doping and electrical characteristics of in-situ heavily B-doped Si1−xyGexCy (0.22<x<0.6, 0<y<0.02) films epitaxially grown on Si(100) were investigated. The epitaxial growth was carried out at 550°C in a SiH4–GeH4–CH3SiH3–B2H6–H2 gas mixture using an ultraclean hot-wall low-pressure chemical vapor deposition (LPCVD) system. It was found that the deposition rate increased with increasing GeH4 partial pressure, and only at high GeH4 partial pressure did it decrease with increasing B2H6 as well as CH3SiH3 partial pressures. With the B2H6 addition, the Ge and C fractions scarcely changed and the B concentration (CB) increased proportionally. The C fraction increased proportionally with increasing CH3SiH3 partial pressures. These results can be explained by the modified Langmuir-type adsorption and reaction scheme. In B-doped Si1−xyGexCy with y=0.0054 or below, the carrier concentration was nearly equal to CB up to approximately 2×1020 cm−3 and was saturated at approximately 5×1020 cm−3, regardless of the Ge fraction. The B-doped Si1−xyGexCy with high Ge and C fractions contained some electrically inactive B even at the lower CB region. Resistivity measurements show that the existence of C in the film enhances alloy scattering. The discrepancy between the observed lattice constant and the calculated value at the higher Ge and C fraction suggests that the B and C atoms exist at the interstitial site more preferentially.  相似文献   

16.
The infrared (IR) absorption spectra and the behavior of the refraction index of a two-phase non-stoichiometric SiO2 film with excess Si have been studied as a function of the excess of Si and post-deposition thermal treatment. The oxides were deposited by low-pressure chemical vapor deposition using SiH4 and N2O as reactant gases at a substrate temperature in the range of 650 to 750 °C. Some of the films were given a final annealing treatment at temperatures ranging from 700 to 1100 °C in N2 for 30 min. Both annealed and as-deposited oxides have IR absorption peaks associated with the bending, rocking and stretching modes of the Si-O-Si bonds in SiO2, although the exact location of these peaks is different for different contents of excess silicon and it also depend on the post-deposition thermal treatment given to the oxides. Unannealed samples present a shift of the stretching peak towards low wavenumbers as the excess of Si is increased. The samples annealed at 1000 °C on the other hand do not present this shift. Unannealed samples with large content of Si also present an absorption peak at 890 cm−1 that could be associated with partially oxidized Si. It is suggested that at least part of the excess Si in the as-deposited samples is present in the form of an SiOx phase while in the annealed samples a clear separation occurs between a Si and a SiO2 phase. The behavior of the refraction index is similar for both types of sample, increasing as the excess silicon is increased.  相似文献   

17.
WSx films were sputter-deposited on Si, SiO2/Si, and glass substrates from a WS2 target in an Ar/H2S atmosphere. Their structure, morphology, chemical composition, and electrical properties were investigated as a function of deposition parameters such as working pressure and H2S fraction. Films could be grown in the composition range WS0.3−WS3.5. Crystallisation was achieved at substrate temperatures Ts > 70 °C and compositions 0.7 ≤ x ≤ 1.95. While the first 5–50 nm near the interface exhibited a basal orientation (c), further growth resulted in the formation of edge-oriented platelets (c) giving rise to a porous, lamellar microstructure. The crystalline structure was mainly turbostratic, while some degree of ordered stacking was present in samples grown at high substrate temperature (600 °C). Resistivity measurements showed a semiconductor-type temperature dependence characterised by activation energies up to 95 meV. Sheet resistance was found to be nearly independent of film thickness, suggesting that the main carrier transport takes place in an interfacial layer of about 20 nm in thickness.  相似文献   

18.
M. Hacke  H. L. Bay  S. Mantl 《Thin solid films》1996,280(1-2):107-111
Silicon molecular beam epitaxy (Si-MBE) has been used to produce silicon oxide (SiOx) films by evaporating Si on a heated Si(100) substrate in an ultra high vacuum system with an O2 pressure of 10−6 to 10−4 mbar. Then the SiOx films were overgrown with pure Si. The influence of the substrate temperature, the O2 pressure and the Si deposition rate on the oxygen content in the SiOx films and on the crystalline quality of the Si top-layer was investigated by Rutherford backscattering spectrometry and ion channeling. Epitaxial growth of the Si top-layer was observed up to a maximum concentration of ≈20 at.% oxygen content in the SiOx film. Cross-sectional transmission electron microscopy shows that the structure of the SiOx film changes duringa subsequent annealing procedure. Electron energy loss spectrometry proves that amorphous SiO2 is formed and the development of holes indicates that the density of the as-grown SiOx film is much lower than that of SiO2. The specific for the as-grown SiOx films was determined by IV measurements.  相似文献   

19.
The effect of N+ implantation on the microstructural and tribological properties of r.f.-sputtered MoS2 films was studied. The cross-section scanning electron micrographs show that, after N+ implantation, the loose column structure of the sputtered MoS2 films increases in density. A decrease in film thickness of about 50% is also observed. The results of X-ray diffraction analysis show that N+ bombardment enhances the (100) edge plane orientation of the MoS2 crystal in the film. The scratch test indicates an improved film-substrate adherence. The tribological test results indicate that N+ implantation yields a distinct enhancement in the wear life of the sputtered MoS2 films. Compared with the as-deposited MoS2 film, the wear life of the sputtered MoS2 films implanted with 150 keV N+ at 1 × 1016 N+ cm−2 shows a threefold increase in a relative humidity of 60%–70% and a twofold increase in a vacuum of 5 × 10−3 Pa. However, N+ implantation inreases the friction coefficient. The lubrication model of the N+-modified film is given.  相似文献   

20.
Atomic-layer doping of P in Si epitaxial growth by alternately supplied PH3 and SiH4 was investigated using ultraclean low-pressure chemical vapor deposition. Three atomic layers of P adsorbed on Si(100) are formed by PH3 exposure at a partial pressure of 0.26 Pa at 450°C. By subsequent SiH4 exposure at 220 Pa at 450°C, Si is epitaxially grown on the P-adsorbed surface. Furthermore, by 12-cycles of exposure to PH3 at 300–450°C and SiH4 at 450°C followed by 20-nm thick capping Si deposition, the multi-layer P-doped epitaxial Si films of average P concentrations of 1021 cm−3 are formed. The resistivity of the film is as low as 2.4×10−4 Ω cm. By annealing the sample at 550°C and above, it is found that the resistivity increases and the surface may become rough, which may be due to formation of SiP precipitates at 550°C and above. These results suggest that the epitaxial growth of very low-resistive Si is achieved only at a very low-temperature such as 450°C.  相似文献   

设为首页 | 免责声明 | 关于勤云 | 加入收藏

Copyright©北京勤云科技发展有限公司  京ICP备09084417号