PbS纳米晶修饰的ZnO/PVP复合电双稳器件阻变机制

采用简单旋涂工艺制备了具有ITO/PVP/ZnO NCs/PbS NCs/PVP/Al 夹心结构的有机/无机复合电双稳存储器件,与没有PbS纳米晶修饰层的器件ITO/PVP/ZnO NCs/PVP/Al相比,PbS纳米晶的引入使目标器件的开关比提高了2个数量级。结合器件的I-V曲线和能级结构分析了PbS 纳米晶修饰层对器件阻变和载流子传输的影响。结果显示,PbS纳米晶层的加入不仅优化了器件能级结构,有利于载流子的俘获和释放,还修饰了ZnO纳米晶的表面缺陷,降低了器件载流子的复合损耗。     

形貌可控的CsPbBr3钙钛矿纳米晶的制备及其形成动力学的原位光致发光研究

通过添加不同比例的十二烷二酸(DDDA)配体,在室温下采用配体辅助再沉淀法制备CsPbBr₃钙钛矿纳米晶.利用X射线衍射仪、透射电子显微镜、紫外分光光度计、荧光光谱仪等对纳米晶的相结构、微结构和光学性质进行了表征.结果显示:所有纳米晶产物均为立方相结构;而纳米晶形貌会随着DDDA浓度的增加从纳米立方块逐渐转变为厚度均一的纳米片,同时光致发光光谱从绿光区移至蓝光区.结合实验室搭建的具有超高时间分辨率(约100 ms)的原位光致发光装置,实时监测了不同形貌纳米晶在形成过程中光致发光光谱的演变.结果表明:未使用DDDA时前驱体经历了快速成核和尺寸分布聚焦生长后生成纳米立方块;DDDA的出现促进了纳米晶在形成早期生成各向异性的纳米片,然而随着反应时间的延长,具有不对称结构的纳米片会通过溶解-再结晶方式转变为热力学稳定的纳米立方块.本工作对形貌可控的钙钛矿纳米晶的精准合成具有一定参考价值.     

水溶性CdTe纳米晶的制备和发光性质的研究

在水相中以巯基乙酸作为稳定剂制备了CdTe纳米晶,用X射线粉末衍射和X射线光电子能谱对其进行了表征,用荧光光谱研究了CdTe纳米晶的生长过程,结果表明,随着回流时间的增加,CdTe半导体纳米晶的粒径和半高全宽逐渐变大,纳米晶的荧光颜色也从绿色逐渐过渡到红色.     

使用SiNx原位淀积方法生长的GaN外延膜中的应力研究

采用低压MOCVD系统,在生长过程中使用SiNx原位淀积的方法产生纳米掩模,并在纳米掩模上进行选区生长和侧向外延制备了GaN外延薄膜.使用拉曼光谱和光荧光的手段对GaN外延膜中的残余应力进行了研究.研究发现,用SiNx原位淀积出纳米掩模后,GaN生长将由二维向三维转变,直到完全合并为止.利用拉曼光谱和光荧光谱分别研究了薄膜中的残余应力,两者符合得很好;这种方法生长出的GaN薄膜的应力分布较传统的侧向外延更加均匀;并且从中发现随着生长过程中SiNx原位淀积时间的增加,生长在其上的GaN外延膜中的残余应力减小.这是因为,随着SiNx原位淀积时间的增加,SiNx纳米掩模的覆盖度也增大.因此侧向外延区的比例增大,残余应力随之减小.     

溶剂热再结晶合成由纳米颗粒自组装成的一维CdS纳米棒

采用两种不同的溶剂热路径合成出了不同形貌和尺寸的CdS纳米晶, 一种是以无水乙二胺(en) 为溶剂, CdCl₂·2.5H₂O和硫脲(H₂NCSH₂N) 为镉源和硫源, 在不同反应温度(160 ℃-220 ℃ 下制备出了CdS纳米晶, 讨论温度对CdS纳米晶生长的影响; 另一种是以en为溶剂, 将在160 ℃下合成的产物在200 ℃下原位再结晶生长2-8 h, 分析原位生长时间对CdS纳米晶生长的影响. 通过X射线衍射(XRD)、 扫描电子电镜(SEM) 和透射电子电镜(TEM) 等表征产物的物相、 形貌和微结构, 分析可知: 两种路线合成的产物均为六方相CdS; 当温度为160 ℃时, 产物形貌为纳米颗粒状, 当温度高于160 ℃时, 产物为CdS纳米棒状; 同时, 在200 ℃下原位再结晶生长不同时间后发现产物形貌由纳米颗粒转变为纳米棒, 通过场发射扫描电镜(HRTEM) 分析可知: 纳米棒是由零维纳米颗粒自组装而成. 最后, 讨论了影响产物CdS纳米晶形貌转变的因素和纳米棒的生长机理.     

热分解含硫金属有机配合物制备近红外PbS量子点

以Pb(NO₃)₂, Na(S₂CNEt₂)·3H₂O为反应物, 在去离子水中合成含硫金属有机配合物Pb(S₂CNEt₂)₂. 氩气保护下, 在油酸和十八烯混合溶液中热分解前躯体Pb(S₂CNEt₂)₂, 反应时间分别为30, 60, 90, 120 min, 获得PbS量子点样品a, b, c, d. 通过红外光谱分析和热重-差热等手段对前躯体进行表征, 证明配体Na(S₂CNEt₂)·3H₂O中的两个硫原子与Pb²⁺配位成功. PbS量子点样品X射线衍射和透射电子显微镜分析表明, 合成的PbS为类球形纯立方晶系PbS纳米晶; 对PbS量子点样品紫外-可见吸收光谱和光致发光谱进行研究发现, 吸收光谱和光致发光谱随着反应时间的增加顺序红移, 表明优化热分解反应时间可以调控PbS量子点的吸收光谱和光致发光谱. PbS量子点样品a发射峰在1080 nm, 与硅基太阳能电池相匹配, 可作为硅基荧光太阳能聚集器的荧光材料. 关键词： 热分解法 含硫金属有机配合物 PbS量子点 反应时间     

使用SiNx原位淀积方法生长的GaN外延膜中的应力研究

采用低压MOCVD系统，在生长过程中使用SiN_x原位淀积的方法产生纳米掩模，并 在纳米掩模上进行选区生长和侧向外延制备了GaN外延薄膜.使用拉曼光谱和光荧光的手段对 GaN外延膜中的残余应力进行了研究.研究发现，用SiN_x原位淀积出纳米掩模后 ，GaN生长将由二维向三维转变，直到完全合并为止.利用拉曼光谱和光荧光谱分别研究了薄 膜中的残余应力，两者符合得很好；这种方法生长出的GaN薄膜的应力分布较传统的侧向外 延更加均匀；并且从中发现随着生长过程中SiN_x原位淀积时间的增加，生长在 其上的GaN外延膜中的残余应力减小.这是因为，随着SiN_x原位淀积时间的增加 ，SiN_x纳米掩模的覆盖度也增大.因此侧向外延区的比例增大，残余应力随之减 小. 关键词： GaN x原位淀积')" href="#">SiN_x原位淀积 拉曼 光荧光 残余应力     

基于等离激元纳腔的单颗粒稀土掺杂纳米晶上转换发光光谱调控

等离激元纳腔可有效调控稀土掺杂纳米晶的上转换发光特性,其不仅能增强上转换发光强度,还可实现上转换发光光谱的调节.然而,目前利用纳腔进行上转化发光光谱调节的研究主要基于系综实验.相比系综实验,单颗粒实验由于可对同一颗上转换纳米晶进行对比研究,因而能够排除系综样品非均匀性对实验的影响.本文基于原子力显微镜原位纳米操纵技术将...     

固/液界面原位红外显微镜和步进扫描时间分辨FTIR反射光谱及其在纳米材料科学中的应用

结合红外显微镜和步进扫描FTIR光谱仪 ,发展了固 /液界面电化学原位显微镜红外反射光谱和步进扫描快速时间分辨FTIR反射光谱 ,并应用于纳米材料特殊性能和电化学反应动力学的研究。研制纳米结构Pt微电极 ,获得CO吸附的红外特征随纳米结构和纳米尺度变化的原位显微镜红外谱图。利用纳米结构Pt微电极的异常红外效应 ,显著提高电化学原位红外反射光谱的灵敏度 ,获得分辨率达 5 0 μs的步进扫描时间分辨光谱。不仅发展了固 /液界面显微镜原位红外反射光谱新方法 ,并且拓展了电化学原位红外反射光谱在纳米材料科学研究中的应用。     

Fe3O4@Au纳米材料的制备和光谱性质

采用共沉淀法制备了Fe3O4纳米颗粒,并以其为晶种利用晶种生长法制备了Fe3O4@Au磁性复合纳米粒子。吸收光谱显示Au壳层成功包覆在了Fe3O4纳米核的表面。以结晶紫为探针分子的表面增强拉曼散射（SERS）光谱展示了Fe3O4@Au良好的SERS活性。     

Luminescence of lead sulfide nanocrystals in a silicate glass matrix

Luminescence of lead sulfide (PbS) nanocrystals with mean diameter 6 nm in a silicate glass matrix that emit in wavelength region 1.5 μm (0.827 eV) is studied. The average luminescence decay time is estimated to be 2.7 μs. Decreasing the temperature is shown to result in a shift of the emission spectrum to lower energies with a corresponding temperature coefficient of 64 μeV/K. Anti-Stokes luminescence of the PbS nanocrystals is detected with a spectral shift of 45 meV for the emission band maximum relative to the excitation energy.     

Optical and structural properties of nanocrystalline PbS thin film grown by CBD on Si(1 0 0) substrate

PbS nanocrystalline thin film was prepared by chemical bath deposition on Si(1?0?0) substrate at bath temperatures of 25, 45 and 65 °C. Triethanolamine was added to the aqueous solution, which decreased the grain size and increased the luminescence of the nanocrystalline PbS thin film. PbS nanocrystals were identified using XRD, TEM and AFM. The crystalline size of the PbS film deposited at different bath temperatures was estimated by XRD and TEM to be 7–12 nm. The growth mechanism of the PbS crystallites were described at different bath temperatures. The confinement was reflected in the absorption spectra, photoluminescence excitation and photoluminescence spectra. The luminescence of Si(1?0?0) substrate and PbS nanocrystalline film deposited on Si(1?0?0) were compared, and the results revealed that the PbS nanocrystals altered and notably enhanced the emission features of the Si(1?0?0) substrate. The shifting of the maximum photoluminescence emission wavelength of PbS nanocrystals with a change in bath temperature and the variation in photoluminescent intensity of PbS nanocrystals prepared at 25 °C versus deposition time were investigated. A single-peak fit of a Gaussian function was employed to discern the photoluminescence of PbS on Si(1?0?0) substrate.     

Oscillations of the absorbance of PbS nanocrystals grown in situ in Langmuir-Blodgett films of lead stearate

Oscillations of the absorbance of PbS nanocrystals point to the high uniformity of their sizes at the stage of “normal” growth in the matrix. The size quantization energies of the ground and the first excited states of an electron-hole pair are analyzed within the effective mass approximation. It is found that the mean radius of PbS nanocrystals is r≈1.7 nm and the potential barrier height at the contact between the semiconductor and the matrix is V _e≈4.5 eV. It is suggested that the finite barrier height is due to the action of electric fields of ～10⁷ V/m in the contact regions upon breaking the polar symmetry of the dipole arrangement of matrix molecules with respect to the surfaces of growing planar nanocrystals.     

The influence of the polymer-stabilizer molecular weight on the spectral luminescence properties of composite sols and coatings containing PbS quantum dots

The influence of the polyvinylpyrrolidone (PVP) molecular weight on the stability and spectral luminescence properties of sols of lead sulfide nanocrystals and the related composite coatings has been studied. It is shown that the spectral properties of PbS sols stabilized with low-molecular (PVP) and the related coatings are determined to a great extent by the formation of large particle aggregates in these materials and, accordingly, high level of light scattering. It is effective to use low-molecular PVP for preparing powder materials containing PbS quantum dots (QDs), because it allows one to perform fast powder precipitation and form small semiconductor particles. High-molecular PVP provides high aggregative and sedimentation stabilities of semiconductor nanocrystal sols. This polymer is effective for use in preparing stable QD sols and homogeneous coatings transparent in the visible spectral range.     

Comparative analysis of Raman spectra of PbS macro- and nanocrystals

A comparative analysis of the Raman spectra of bulk PbS and PbS nanocrystals with average diameters of 6.6 and 3.8 nm has been performed. It is shown that the bands due to the LO phonons at the Γ point of the Brillouin zone dominate in the first- and second-order Raman spectra of the nanocrystals. Based on the analysis of the relative band intensities for the first- and second-order spectra a qualitative conclusion is drawn: the electron-LO-phonon interaction in PbS nanocrystals increases with a decrease in their size.     

Polymer-assisted crystallization of low-dimensional lead sulfide particles

PbS micro- and nanoparticles were synthesized by a simple precipitation reaction of lead nitrate with thioacetamide in hydrosoluble polymer water solutions. The effects of four water soluble polymers: polyacrylamide (PAM), polyvinyl alcohol (PVA), polyethylene glycol (PEG) and poly-N-vinyl pyrrolidone (PVP) on the PbS crystallites morphology and structural properties were investigated by scanning electron microscopy (SEM) and X-ray diffraction (XRD). It was found that for the PbS particles obtained in the PVA, PEG and PVP, the (2 0 0) diffraction peak of the nanocrystals becomes dominant. The highest texture in the [2 0 0] direction was observed for the crystallites obtained in the presence of PVP. Polydisperse PbS particles with cubic morphology and size ranging from 100 nm to several microns are obtained in the case of PAM and PEG. Monodisperse cubic PbS crystallites with an average size of 200 nm are formed in the presence of PVA and PVP.     

Growth and characteristics of lead sulfide nanocrystals produced by the porous alumina membrane

Lead sulfide (PbS) nanocrystals were formed by using Pb nanowires reacted with hydrogen sulfide (H₂S) gas. The structure and composition of the as-prepared nanocrystals were confirmed by scanning electron microscopy, X-ray diffraction, transmission electron microscope and energy dispersive X-ray spectroscopy. According to the differential scanning calorimeter analysis, the PbS nanocrystals in a cubic structure owned excellent thermal stability. Furthermore, the optical properties including photoluminescence (PL) and Raman scatting spectrum were also measured. The PL emission measurement of the PbS nanocrystal showed that there was an orange-red emission peak located around 655 nm. A significant quantum confinement effect made the energy gap of PbS produce a blue shift from 0.41 eV to 1.9 eV.     

Room-temperature amplified spontaneous emission at 1300 nm in solution-processed PbS quantum-dot films

We report room-temperature amplified spontaneous emission and spectral narrowing at infrared wavelengths in solution-processed films made up of PbS quantum-dot nanocrystals. The results are relevant to optical amplification and lasing integrated upon a variety of substrates. The active optical medium operates at room temperature without any additional matrix material, providing an optical gain of 260 cm(-1) and a pump threshold of 1 mJ/cm(-2). Nanocrystals synthesized in an aqueous solution and stabilized by use of short ligands result in high quantum-dot volume fractions in solid films and in a redshift emission relative to absorption.     

Lead sulfide colloidal nanocrystals with strong optical nonlinearity

Colloidal PbS nanocrystals have been synthesized by a developed procedure. UV–Vis absorption and Z-scan technique was also applied to study the nonlinear optical properties of prepared lead sulfide nanocrystals at 532 nm wavelength. The nonlinear refractive (n₂) and absorption (β) were determined which are confirming the strong nonlinearity at 532 nm of colloidal PbS nanocrystals. The obtained results have not been reported before. In this study, only a weak thermal optical nonlinearity was observed and the dominating nonlinear response is resulted by the electronic origin. The nonlinear optical properties of prepared sample supported wide applications in nanophotonics.     

Measurement of the luminescence decay times of PbS quantum dots in the near-IR spectral range

Methods for recording luminescence decay times of semiconductor PbS quantum dots (QDs) with optical transitions in the near-IR spectral range have been analyzed. A measuring complex for spectral and kinetic analysis in the near-IR range (0.8?C2.0 ??m) in the time interval from several tens of nanoseconds to several tens of microseconds is described. In this complex, a semiconductor picosecond laser is used as an excitation source; luminescence decay times are recorded by a fast InGaAs photodiode, a high-speed amplifier, and a high-frequency oscilloscope; and the measurement results are multiply averaged (up to a million times) by a program. The technical features of this method are discussed and compared with the characteristics of techniques based on photon counting or application of more powerful radiation sources, and the limitations on sensitivity are analyzed. The results of measuring the luminescence decay kinetics of PbS QDs 2.7?C7.6 nm in size prepared in the form of solutions and incorporated into matrices are reported.