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1.

Colloidal nanocrystals of CuInS2 and CuInSe2 were synthesized in an apolar noncoordinating medium using 1-dodecanethiol as a ligand. A semiconductor shell of ZnS was formed for CuInS2 nanocrystals obtained by the injection method. The obtained samples were characterized by absorption spectroscopy and photoluminescence.

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2.
2 nanocrystals in a polymer film have been studied with the picosecond pump-probe technique. The oxidized CuInS2 nanocrystals have an additional absorption band with a peak at 1.03 eV, which is bleached under picosecond excitation. Rapid (∼50 ps) trapping into midgap surface states results in long-lived (≫300 ps) bleaching and induced absorption features. A schematical energy-level diagram for oxidized CuInS2 nanocrystals is given based on the experimental results. Received: 7 January 1997/Revised version: 16 April 1997  相似文献   

3.
于丹阳  小林康之  小林敏志 《物理学报》2012,61(19):198102-198102
采用直流三极溅射装置制备获得了CuInS2薄膜, 其中溅射靶采用一定面积比的[Cu]/[In]混合靶,反应气体采用CS2气体. 本文中主要研究了0.02 Pa分压反应气体条件下不同面积比的[Cu]/[In]混合靶和沉积基板温度对CuInS2薄膜结构和成分的影响, 其中CuInS2薄膜制备所用时间为2 h生长的厚度为1—2 μm. 通过对CuInS2薄膜的EPMA, X射线衍射测试分析表明, 最佳的CuInS2薄膜可在面积比[Cu]/[In]混合靶为1.4:1和可控温度(150, 250和350 ℃)的条件下制备获得, 并且其结构被确认为黄铜矿结构. 通过实验结果计算出CuInS2薄膜层有约为8.9%的C杂质含量.  相似文献   

4.
CuInS2 (CIS) nanocrystals were successfully synthesized through a hot-injection technique employing a reaction of copper (I) acetate and indium (III) acetate with tert-dodecanethiol as a source of sulfur, and trioctylphosphine oxide and 1-dodecanethiol were used as ligands. The reaction medium was a mixture of two solvents: oleylamine and 1-octadecene. Varying the ratio between both solvents leads to the formation of wurtzite CuInS2 particles with shapes ranging from triangular to rod-shaped with length up to 50 nm. Oleylamine turned out to influence the reaction condition in two opposite ways: by leading to monomer depletion before the injection of the sulfur precursor, and at the same time increasing the activity of the monomers remaining in solution. By changing the sulfur source from tert-dodecanethiol to sulfur dissolved in oleylamine, triangular particles with zinc blend structure and a smaller size (~5 nm) were synthesized. The final materials were characterized by powder X-ray diffraction (XRD), transmission electron microscopy (TEM), energy dispersive X-ray analysis (EDX), and absorption spectroscopy (UV?CVis).  相似文献   

5.
CuIn(SxSe1−x)2 thin polycrystalline films were grown by the chemical spray pyrolysis method on the glass substrate at 280-400°C. The alloy composition in the film was studied with relation to that in the splay solution. Films were characterized by X-ray diffraction, optical absorption, Raman spectroscopy, resistivity and surface morphology. The CuInSe2-rich alloy films grown at high substrate temperature had chalcopyrite structure, while, the CuInS2-rich films grown at low substrate temperature exhibited sphalerite structure. Optical-gap energies were smaller than that of the bulk crystal by 0.1-0.2 eV for CuInS2-rich films. Raman spectra exhibited both CuInSe2-like and CuInS2-like A1 modes, and their relative changed systematically with alloy composition.  相似文献   

6.
Glasses are obtained that contain CuInS2 nanoparticles dispersed in a silicate matrix. The absorption and luminescence spectra of the glasses containing CuInS2 nanocrystals with particle dimensions of 10–70 nm are studied. The possible reasons for the longwave shift of the fundamental absorption edge and inconsistency of the crystal structure of the CuInS2 nanoparticles with a chalcopyrite lattice are discussed. Translated from Zhurnal Prikladnoi Spektroskopii, Vol. 65, No. 3, pp. 387–393, May–June, 1998.  相似文献   

7.
CuInS2 thin films were prepared by a two-stage ion layer gas reaction (ILGAR) process in which the Cu and In precursors were deposited on glass substrate by using a simple and low-cost dip coating technique and annealed in H2S atmosphere at different temperatures. The influence of the annealing temperature (250-450 °C) on the particle size, crystal structure and optical properties of the CuInS2 thin films was studied. Transmission electron microscopy revealed that the particle radii varied in the range 6-21 nm with annealing. XRD and SAED patterns indicated polycrystalline nature of the nanoparticles. The optical band gap (Eg) varied from 1.48 to 1.56 eV with variation of particle size. The variation of Urbach tail with temperature indicated higher density of the defects for the films annealed at lower temperature. From the Raman study, it was observed that the FWHM of the A1 mode at ∼292 cm−1 corresponding to the chalcopyrite phase of CuInS2 decreased with increasing annealing temperature.  相似文献   

8.
The growth of polycrystalline CuInSe2 and CuInS2 thin films from metallic precursor layers is investigated using two complementary in situ methods which give bulk sensitive (XRD) and surface sensitive (Raman) information. From the time evolution of the XRD and Raman peak intensities the phase transformation sequences and the reaction kinetics can be derived. In both cases the chalcogenization of the Cu-In precursors proceeds at the top surface. Thus, the process is at least limited by cation diffusion through the metallic precursor. However, the growth kinetics of CuInSe2 and CuInS2 films differ. While the CuInSe2 growth is limited by the reaction of binary phases, CuInS2 growth is controlled by fast diffusion which is solely restricted to the period of raising temperature during the process.  相似文献   

9.
Picosecond time‐resolved X‐ray diffraction has been used to study the nanoscale thermal transportation dynamics of bare gold nanocrystals and thiol‐based self‐assembled monolayer (SAM)‐coated integrated gold nanocrystals on a SiO2 glass substrate. A temporal lattice expansion of 0.30–0.33% was observed in the bare and SAM‐coated nanocrystals on the glass substrate; the thermal energy inside the gold nanocrystals was transported to the contacted substrate through the gold–SiO2 interface. The interfacial thermal conductivity between the single‐layered gold nanocrystal film and the SiO2 substrate is estimated to be 45 MW m?2 K?1 from the decay of the Au 111 peak shift, which was linearly dependent on the transient temperature. For the SAM‐coated gold nanocrystals, the thermal dissipation was faster than that of the bare gold nanocrystal film. The thermal flow from the nanocrystals to the SAM‐coated molecules promotes heat dissipation from the laser‐heated SAM‐coated gold nanocrystals. The thermal transportation of the laser‐heated SAM‐coated gold nanocrystal film was analyzed using the bidirectional thermal dissipation model.  相似文献   

10.
CuInS2 ternary films were prepared by a soft solution processing, i.e. successive ionic layer absorption and reaction (SILAR) method. The films were deposited on glass substrates at room temperature and heat-treated under Ar atmosphere at 500 °C for 1 h. CuCl2 and InCl3 mixed solutions with different ionic ratios ([Cu]/[In]) were used as cation precursor and Na2S as the anion precursor. The effect of the [Cu]/[In] ratio in precursor solution on the structural, chemical stoichiometry, topographical, optical and electrical properties of CuInS2 thin films was investigated. XPS results demonstrated that stoichiometric CuInS2 film can be obtained by adjusting [Cu]/[In] ratios in solution. Chalcopyrite structure of the film was confirmed by XRD analysis. The near stoichiometric CuInS2 film has the optical band gap Eg of 1.45 and resistivity decreased with increase of [Cu]/[In] ratios.  相似文献   

11.
Structural, electrical and optical properties of Sb-doped CuInS2 thin films grown by single source thermal evaporation method were studied. The films were annealed from 100 to 500 °C in air after the evaporation. The X-ray diffraction spectra indicated that polycrystalline CuInS2 films were successfully obtained by annealing above 200 °C. This temperature was lower than that of non-doped CuInS2 films. Furthermore, We found that the Sb-doped CuInS2 thin films became close to stoichiometry in comparison with non-doped CuInS2 thin films. The Sb-doped samples annealed above 200 °C has bandgap energy of 1.43–1.50 eV.  相似文献   

12.
ZnO nanorods with a cone and different aspect ratios and short-and-fat ZnO microrods were synthesized via a hydrothermal reaction of Zn with Zn(CH3COO)2 and H2O. The control over these ZnO nanocrystals with a wurtzite structure and different shapes was achieved by adjusting only the reaction temperature and time. A possible kinetic mechanism was proposed to account for the growth of these ZnO nanocrystals with different shapes. Photocatalytic activities of ZnO nanocrystals with distinctive shapes in the degradation of methyl orange were investigated. The results indicate that the photocatalytic ability of the ZnO nanorods with a cone and different aspect ratios is stronger than that of the short-and-fat microrods.  相似文献   

13.
提出了一种通过反应烧结来制备CuInS2多晶薄膜的低成本旋涂工艺路线.通过将前驱物粉末在氢气中预还原的方法来优化旋涂时使用的墨水成分,氢气还原会使前驱物纳米粉末从硫化物混合粉末转变成CuInS2和Cu-In合金的混合物.扫描电子显微镜、电子能谱、X射线衍射以及拉曼图谱的结果表明,这种优化能极大的提高CuInS2多晶薄膜的性能,其中包括薄膜的排列密度更高,杂质相减少,薄膜质量变得更好等.吸收光谱测得优化后的铜铟硫薄膜的带隙约为1.45 eV.  相似文献   

14.
In this study CuInSe2 and CuInS2 thin films were prepared onto ITO glass substrate using the electrodeposition technique in aqueous solution. The electrodeposited films were characterized by X-ray diffraction (XRD), scanning electron microscopy (SEM) and energy dispersive X-ray analysis. The annealing effects on electrodeposited precursors were investigated. The chalcopyrite structure of CuInSe2/CuInS2 showed an enhancement of crystallinity after subsequent selenization/sulfurization treatment in Se/S atmosphere, respectively. XRD and SEM studies revealed a dramatic improvement of the crystalline quality of CIS films after annealing treatments. Mott–Schottky measurements were used to assess the conductivity type of the films and their carrier concentration. The prepared samples underwent an etching process to remove the binary accumulated Cu2?x(Se,S) phases shown in FESEM pictures. This etching process has shown a noticeable decrease in both, the flat band potential, Vfb (V), and the number of acceptors, NA (cm?3) in selenized CuInSe2 and sulfurized CuInS2 samples.  相似文献   

15.
Large scale of uniform small ZnWO4 nanocrystals and ZnWO4 nanorods with tunable size have been fabricated in ethylene glycol (EG)-assisted solvothermal process, ZnWO4 samples ranging in shape from tiny nanocrystals to nanorods were dependent on the volume ratio of EG and water (H2O). The optical properties of ZnWO4 nanocrystals and nanorods were investigated by photoluminescence (PL) spectroscopy, showing longer ZnWO4 nanorods own the increased PL intensity in comparison with that of shorter ones and small ZnWO4 nanocrystals. The photocatalytic performance of ZnWO4 nanostructures was studied also, which indicated that the increased size of ZnWO4 nanorods resulted the degradation of photocatalytic performance in aqueous solution.  相似文献   

16.
Thin CuInS2 light-absorbing layer prospective for the solar cell applications is modified by gold nanoparticles. Theoretical and experimental possibilities of placement nanoparticles over or under the CuInS2 coating were tested. It was revealed that placement of nanoparticles under the CuInS2 layer is better in terms of spray pyrolysis technique. It results in more effective plasmon-enhanced light absorption in the CuInS2 layer at the visible/near infrared 650–700 nm spectral range.  相似文献   

17.
Mn-doped ZnS nanocrystals prepared by solvothermal method have been successfully coated with different thicknesses of Zn(OH)2 shells through precipitation reaction. The impact of Zn(OH)2 shells on luminescent properties of the ZnS:Mn nanocrystals was investigated. X-ray diffraction (XRD) measurements showed that the ZnS:Mn nanocrystals have cubic zinc blende structure. The morphology of nanocrystals is spherical shape measured by transmission electron microscopy (TEM). ZnS:Mn/Zn(OH)2 core/shell nanocrystals exhibited much improved luminescent properties than those of unpassivated ZnS:Mn nanocrystals. The luminescence enhancement was observed with the Zn(OH)2 shell thickening by photoluminescence (PL) spectra at room temperature and the luminescence lifetime of transition from 4T1 to 6A1 of Mn2+ ions was also prolonged. This result was led by the effective, robust passivation of ZnS surface states by the Zn(OH)2 shells, which consequently suppressed nonradiative recombination transitions.  相似文献   

18.
CuInS2, CuInSe2 and CuInTe2 nanocubes of chalcopyrite structure have been successfully synthesized by hydrothermal process using deionized water as solvent at 180 °C for 20 h. The crystallinity, compositional, morphological and optical properties of the synthesized samples were studied by X-ray diffraction (XRD), scanning electron microscopy (SEM), transmission electron microscopy (TEM), energy dispersive X-ray (EDX), Raman and photoluminescence (PL) spectra analyses. The Raman spectra of the synthesized CuInS2, CuInSe2 and CuInTe2 samples show the dominant A1 modes at 293, 172 and 121 cm−1 respectively. The possible chemical reaction and mechanism of nanocubes formation were discussed. The emission wavelength of as synthesized CuInS2, CuInSe2 and CuInTe2 samples were blue shifted at 746 nm (1.66 eV), 863 nm (1.43 eV) and 859 nm (1.44 eV) respectively.  相似文献   

19.
Summary A theoretical analysis has been carried out to investigate the kinetics involved in the CVD growth of CuInS2. A stagnant-layer model is assumed for the numerical, simulation. Computational results for the growth rate as a function of the substrate temperature, mean, gas velocity and partial pressures in the reaction tube are obtained. This analysis indicates that the substrate temperature plays a dominant role in the growth rate, which is consistent with our experimental data. Paper presented at the ?V International Conference on Ternary and Multinary Compounds?, held in Cagliari, September 14–16, 1982.  相似文献   

20.
Temperature-dependent photoluminescence (PL) spectroscopy of CuInS2 core and CuInS2/ZnS core–shell quantum dots (QDs) was studied for understanding the influence of a ZnS shell on the PL mechanism. The PL quantum yield and lifetime of CuInS2 core QDs were significantly enhanced after the QD surface was coated with the ZnS shell. The temperature dependences of the PL energy, linewidth, and intensity for the core and core–shell QDs were studied in the temperature range from 92 to 287 K. The temperature-dependent shifts of 98 meV and 35 meV for the PL energies of the QDs were much larger than those of the excitons in their bulk semiconductors. It was surprisingly found that the core and core–shell QDs exhibited a similar temperature dependence of the PL intensity. The PL in the CuInS2/ZnS core–shell QDs was suggested to originate from recombination of many kinds of defect-related emission centers in the interior of the cores.  相似文献   

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