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1.
Abstract

We have found recently that thin film layered heterojunction between C60 and conducting polymer, like poly(3-alkylthiophene) (PAT) shows a photovoltaic effect due to photoinduced charge transfer at the interface. Here we describe two other examples of such photocells in RO-PPV/C60 and PPP/C60 heterojunctions and study their spectral characteristics. Contrary to conventional inorganic semiconductor p-n junction photocells, the C60-PAT junction can be rather viewed as molecular donor-acceptor (D-A) type photocell in which the processes of photogeneration and separation of charge carriers are quite distinct. In a p-n junction free electron-hole pairs are known to be primarily photogenerated at interband transition and then separated in the internal electric field of the barrier, while in D-A molecular photocell mainly neutral excitons are first created by light, with charges being primarily separated at the narrow interface region due to D-A type intermolecular charge transfer interactions. We analyze how this processes depend on the wavelength of the pumping light and on the polarity and magnitude of the applied voltage.  相似文献   

2.
Lead titanate powders and thin films were prepared by the sol-gel process of metal alkoxide solutions and solvents. From DSC measurements, phase transition temperature of crystallized PbTiO3 powders was obtained at about 484 °C. From XRD investigation, it was confirmed that the tetragonal phase of polycrystalline PbTiO3 thin films is formed by coating of concentrated solution on all of the substrates we used after heat treatment above 500 °C. It was found by SEM and ellipsometric analysis that the thin film coated with 0.25 M concentrated solutions once had an average thickness of about 720 Å. Surfaces of thin films were crack-free, uniform, and its average grain size investigated by SEM was 0.6–0.8 μm. Band gap energy of PbTiO3 thin film coated on the Al2O3 (2243) substrate was 3.45 eV, which is assumed to be due to the direct band to band transition. Dielectric constant (ϵ) and dielectric loss (tan δ) of PbTiO3 thin film amounted to 60–70 and 0.01–0.02 in the region of 10 kHz ∼ 1 MHz at room temperature, respectively, and transition temperature was 486 °C at 1 MHz. From the hysteresis loop of PbTiO3 thin film, spontaneous polarization of 12 μC/cm2 and coercive filed of 45 kV/cm were obtained.  相似文献   

3.
4.
Dislocation structure of GexSi1?x films (x=0.4?0.8) grown by molecular-beam epitaxy on Si(001) substrates was studied by means of transmission electron microscopy. It was found that the density of edge MDs formed at the early stage of plastic strain relaxation in the films could exceed the density of 60° MDs. In our previous publications, a predominant mechanism underlying the early formation of edge misfit dislocations (MD) in GexSi1?x/Si films with x>0.4 was identified; this mechanism involves the following processes. A 60° glissile MD provokes nucleation of a complementary 60° MD gliding on a mirror-like tilted plane (111). A new edge MD forms as a result of interaction of the two complementary 60° MDs, and the length of the newly formed edge MD can then be increased following the motion of the “arms” of the complementary 60° MDs. Based on this scenario of the edge MD generation process, we have calculated the critical thickness of insertion of an edge MD into GeSi layers of different compositions using the force balance model. The obtained values were found to be more than twice lower than the similar values for 60° MDs. This result suggests that a promising strategy towards obtaining dislocation arrays dominated by 90° dislocations in MBE-grown GexSi1?x/Si films can be implemented through preliminary growth on the substrate of a thin, slightly relaxed buffer layer with 60° MDs present in this layer. The dislocated buffer layer, acting as a source of threading dislocations, promotes the strain relaxation in the main growing film through nucleation of edge MDs in the film/buffer interface. It was shown that in the presence of threading dislocations penetrating from the relaxed buffer into the film nucleation of edge MDs in the stressed film can be initiated even if the film thickness remains small in comparison with the critical thickness for insertion of 60° MDs. Examples of such unusual MD generation processes are found in the literature.  相似文献   

5.
Bi‐based oxide thin films are important superconducting materials because of its wide applicability, high transition temperatures, and low toxicity. To achieve high quality Bi‐based oxide thin films by molecular beam epitaxy (MBE), the composition is a key parameter. Here, Bi, Cu, Cu/Sr and Cu/Ca thin films on glass substrates prepared by MBE have been examined by using both X‐ray reflectivity and surface profiler. The thickness and surface roughness were obtained through calculation and simulation. In comparison with the film thicknesses measured by these two methods, they are in good agreement. The lines of thickness deposition rate (R) versus source temperature (T) are according with LogR=a+b/T based on Clausius‐Clapeyron equation. Moreover, the Bi2.1CaySr1.9‐yCuO6+δ thin films with different composition and thickness were successfully prepared by MBE by applying the thickness deposition rate lines. (© 2011 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)  相似文献   

6.
Quaternary compound Cu2ZnSnSe4 (CZTSe) is one of the most promising absorber layer materials for thin film solar cells. In present work, the CZTSe nanocrystals were successfully synthesized via one pot route, and the influences of reaction temperature on the structural, compositional, morphological and optical properties of as‐synthesized CZTSe nanocrystals were investigated in detail via X‐ray powder diffraction (XRD), energy dispersive X‐ray spectrometry (EDS), transmission electron microscopy (TEM) and UV‐Vis spectrophotometry, respectively. The characterization results of as‐synthesized nanocrystals, under optimal synthesis condition (250 °C, 1 h), indicated that the nanocrystals was monodispersed with polycrystalline, the size was in the range of 10–15 nm, and the band gap energy was around 1.44 eV which is very closed to the best band gap energy for the solar cell. All results suggested that the as‐synthesized CZTSe nanocrystals were good light absorber layer material for thin film solar cell.  相似文献   

7.
Abstract

The interaction between C60 and Si atoms was investigated using X-ray photoelectron spec-troscopy (XPS) for the photo-irradiated Si-deposited C60 film in order to establish a method of a synthesis for the Si-coated C60. It was found that the Cls spectrum of the photo-irradiated film contains a peak due to C-Si bonding, while no peak due to C-Si bonding was observed for the film before photo-irradiation. This indicates that Si atoms stick to C60 when using the present method.  相似文献   

8.
Thermally processed lead iodide (PbI2) thin films were prepared by the vacuum evaporation method in a constant ambient. Measured thickness of the film was verified analytically from the optical transmittance data in a wavelength range between 300 and 1600 nm. From the Tauc relation for the non‐direct inter band transition, the optical band gap of the film was found to be 2.58 eV for film thickness 300 nm. X‐ray diffraction analysis confirmed that PbI2 films are polycrystalline, having hexagonal structure. The low fluctuation in Urbach energy indicates that the grain size is quite small. The present findings are in agreement with the other results. (© 2008 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)  相似文献   

9.
Copper thin films (5–150 nm) were prepared by vacuum deposition with different rates (0.7, 1.5 and 3 nm/s). The position, intensity and profile of X-ray diffraction lines were analysed to study the phases, the crystallographic preferred orientation as well as the residual strain and crystallite size. The fcc polycrystalline Cu phase was revealed and no oxide phases were identified. The films were highly oriented with 〈111〉 fiber texture. The ratio of P111/P200 increased with the film thickness. Thus, in case of amorphous substrate, the type of the crystallographic texture of a film depends mainly on the structure of the deposited material. The crystallite size increases while the residual strain decreases, as the film thickness or the deposition rate is increased. The crystallite size was very small compared with the film thickness. The effect of deposition rate was pronounced specially from 0.7 to 1.5 nm/s.  相似文献   

10.
Nanocomposite SiO2(Si) films containing Si nanocrystals (NCs) in a SiO2 dielectric matrix obtained through (i) plasma enhanced chemical vapor deposition (PE CVD) or (ii) pulse laser deposition (PLD) have been investigated as a medium for charge storage. The CV method was used to characterize charging effects in the MIS structure (capacitor) with a nanocomposite SiO2(Si) film as an insulator. The obtained results indicate (i) the capture of small negative charge at the positive gate voltage in the nanocomposite SiO2(Si) film, (ii) significant capture of positive charge at the negative gate voltage, and that (iii) the difference between the positive and negative charge captured in both cases cannot be explained by dropping a part of the positive gate voltage in the semiconductor’s depletion region. A model of charge transport and capture in nanocrystals of nanocomposite SiO2(Si) film is proposed to explain the experimental results.  相似文献   

11.
A silicon oxide thin film barrier was prepared with various oxygen contents and its chemical composition, surface morphology and optical and barrier properties were related to the deposition conditions used. Our study showed that under Ar and O2 assisted process conditions, a stoichiometric silicon oxide thin film formed at a critical oxygen content during deposition of 40-50%. The thin films deposited at the critical condition showed the lowest surface roughness giving similar or higher optical transmittance than that of the bare polycarbonate (PC) substrate. The boiling and tensile strength test performed on the thin film deposited with assisted ions before the deposition process showed improvement in the adhesion between the oxide layer and the polymer substrate. In addition, interface modification to improve for improving the barrier layer properties of the silicon oxide thin film was achieved through the introduction of dual ion beam sputtering without pre-treatment.  相似文献   

12.
a-Si1?xCx:H films are deposited by RF plasma enhanced chemical vapor deposition (PECVD) at different RF powers with hydrogen-diluted silane and methane mixture as reactive gases. The structure and properties of the thin films are measured by infrared spectroscope (IR), Raman scattering spectroscope and ultra violet–visible transmission spectroscope (UV–vis), respectively. Results show that the optical band gap of the a-Si1?xCx:H thin films increases with increasing Si–C bond fraction. It can be easily controlled through controlling Si–C bond formed by modulating deposition power. At low deposition power, the bond configuration of the a-Si1?xCx:H thin film is more disordered owing to the distinct different bond lengths and bond strengths between Si and C atoms. At a too high deposition power, it becomes still high disordered due to dangling bonds appearing in the a-Si1?xCx:H thin film. The low disordered bond configuration appears in the thin film deposited with moderate deposition power density of about 2.5 W/cm2.  相似文献   

13.
Spindle‐shaped α‐FeOOH nanocrystals were facilely synthesized using a poly (vinyl pyrrolidone) (PVP)‐assisted route under hydrothermal conditions. The chemical compositions and morphol‐ogies of the as‐prepared samples were characterized in detail by X‐ray power diffraction (XRD), scanning electron microscopy (SEM), and transmission electron microscope (TEM). The experimental results reveal that these spindle‐shaped α‐FeOOH nanocrystals have self‐organized into assemblies with hierarchical nanostructures. The crucial roles of PVP in the hydrothermal synthesis of hierarchical α‐FeOOH nanostructures were discussed. The possible formation mechanism was also suggested. Moreover, the spindle‐shaped α‐Fe2O3 nanocrystals could be easily obtained after calcining the α‐FeOOH prepared by the PVP‐assisted hydrothermal process. (© 2011 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)  相似文献   

14.
ZrO2-SiO2 binary films for active optical waveguides were prepared by the sol-gel method with zirconium oxychloride and tetraethoxysilane as precursors. The main factors that influence the film thickness and refractive index have been found. The relationship between the film refractive index composition and heat treatment temperature has been determined. The continuous tuning of the thickness and refractive index of the thin films has also been achieved, which will open up new possibilities in the development of active optical waveguides.  相似文献   

15.
The growth of C60 nanowhiskers (C60NWs) prepared by a modified liquid–liquid interfacial precipitation method is investigated, focusing on the effect of solvent ratio and water content in the C60–toluene–isopropyl alcohol (IPA) solution system. The precipitation of C60NWs was markedly influenced by the solvent ratio of toluene to IPA, and the C60NWs were found to grow longer above a critical diameter (Dc), which depends on the solvent ratio. The addition of a small amount of H2O to the C60–toluene–IPA solution promoted the growth of C60NWs. This catalytic effect of water on the growth of C60NWs was confirmed also by the experiment using heavy water (D2O) and by the decrease of growth activation energy of C60NWs with increase of H2O content in the C60–toluene–IPA solution.  相似文献   

16.
《Journal of Crystal Growth》2003,247(1-2):105-109
Y-type magnetoplumbite (Ba2Co2Fe12O22:Co2Y) epitaxial thin films with such a huge lattice parameter as 43.5 Å have been synthesized for the first time. Combinatorial thin film technology was successfully employed to eliminate an impurity phase in the film by quickly optimizing such reaction parameters as the deposition temperature and the thickness of pre-deposition of CoO layer. The coupling of combinatorial pulsed laser deposition and subsequent concurrent X-ray diffraction, both of which we have developed, is a promising way to high throughput optimization of thin film growth and properties.  相似文献   

17.
Titanium silicide thin films were prepared on glass substrates by chemical vapor deposition using SiH4 and TiCl4 as the precursors. The phase structure of the thin films was identified by XRD. The surface morphology of the thin films was observed by FESEM. The sheet resistance and optical behaviors of the thin films were measured by the four point resistivity test system and FTIR spectrometer, respectively. Titanium disilicide (TiSi2) thin films with the face-centered orthorhombic structure are formed. The suitable formation temperature of the TiSi2 crystalline phase is about 710 °C. The formation of TiSi2 crystalline phase is dependent on the thickness of thin films and a quantity of the crystalline phase of TiSi2 in the thin film is directly related to mole ratio of SiH4/TiCl4. The sheet resistance of the TiSi2 thin films is dependent on the formation of the TiSi2 crystalline phase. With the mole ratio of SiH4/TiCl4 of 3, the lowest sheet resistance (0.7 Ω/□) of titanium silicide thin film is formed at 710 °C. The maximum reflectance of the TiSi2 thin films is about 0.95 on the broad IR heat radiation. A related reaction mechanism was proposed.  相似文献   

18.
《Journal of Crystal Growth》2006,286(2):481-486
Tungsten disulfide (WS2) films were obtained by solid state reaction of spray deposited WO3 with gaseous sulfur i.e. solid gas phase reaction (SGP). The XRD and SEM studies revealed the formation of WS2 thin films on quartz substrate with a mixed type-I and type-II texture. The WS2 thin films prepared with a controlled heating/cooling rate of 323 K/h. during the sulfurization were free from cracks while those prepared with higher heating/cooling rate during the sulfurization suffer from cracks. The former WS2 thin film comprises well defined hexagonal crystallites with larger size (2 μm) and thickness. The complete conversion of WO3 into WS2 was observed when sulfurization carried out in evacuated quartz ampoule containing sulfur. A low oxygen and carbon content was observed in XPS spectrum due to air exposure of the sample which is removed by in-situ Ar cleaning. XPS and EDS studies showed that the films are stoichiometric.  相似文献   

19.
Undoped ZnO films were deposited by radio frequency (RF) magnetron sputtering on amorphous buffer layers such as SiOx, SiOxNy, and SiNx prepared by plasma enhanced chemical vapor deposition (PECVD) for dielectric layer in thin film transistor (TFT) application. ZnO was also deposited directly on glass and quartz substrate for comparison. It was found that continuous films were formed in the thickness up to 10 nm on all buffer layers. The crystallinity of ZnO films was improved in the order on quartz>SiOx >SiOxNy>glass>SiNx according to the investigated intensities of (0 0 2) XRD peaks. The crystallite sizes of ZnO were in the order of SiOx~glass >SiNx. Stable XRD parameters of ZnO thin films were obtained to the thickness from 40 to 100 nm grown on SiOx insulator for TFT application. Investigation of the ZnO thin films by atomic force microscope (AFM) revealed that grain size and roughness obtained on SiNx were larger than those on SiOx and glass. Hence, both nucleation and crystallinity of sputtered ZnO thin films remarkably depended on amorphous buffer layers.  相似文献   

20.
Abstract

The structural modification induced by electron-beam (EB) in a C60 film and its kinetics have been studied using in situ high-resolution FT-IR spectroscopy. Similar to studies on photoirradiated KxC60 fim, was found that a coalescence reaction between adjacent C60 molecules takes place. In order to investigate the interaction between an incident electron and Cgg molecules, the time-dependence of the amounts of C60 on the EB irradiation was examined. It was found that the reaction rate exhibits a linear dependence on the reactant concentration and nonlinear dependence on the incident current.  相似文献   

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