利用P-MBE制备高质量MgxZn1-xO的结构和光学特性

利用等离子体辅助分子束外延(P-MBE)的方法,在c平面的蓝宝石衬底上制备了高质量的MgxZn1-xO合金薄膜。通过改变Mg源的温度,得到了不同Mg组份的MgxZn1-xO合金薄膜;通过引入ZnO的低温缓冲层,有效地提高了MgxZn1-xO合金薄膜的结晶质量。随着Mg组份的增加,MgxZn1-xO的X射线衍射的(002)衍射峰逐渐向大角度方向移动。对样品进行光致发光(PL)谱的测量,在室温下观察到了较强的紫外发光。随Mg浓度的增加,紫外发光峰向高能侧移动,并且发光峰逐渐展宽。通过对x=0.15的样品进行变温光谱的测量研究了紫外发光峰起因,得到了MgxZn1-xO的发光是来自于自由激子的发光。自由激子束缚能为54meV。     

火焰喷雾法合成ZnO和MgxZn1-xO纳米颗粒的光学性能研究

利用火焰喷雾法成功制备了纳米级的ZnO和Mgxzn1-xO颗粒.通过对样品的X射线衍射谱和场发射扫描电子显微镜照片分析,发现制备的颗粒大小较为均匀,直径在20 nm左右;镁元素的掺入引起晶格常数变小.通过透射光谱和光致发光谱的测量,发现MgxZn1-xO颗粒的禁带宽度远大于ZnO颗粒的禁带宽度,同时对两组样品的紫外发光和可见发光的强度变化和发光机理进行了探讨.     

MgxZn1-xO/Au/MgxZn1-xO夹层透明导电薄膜的制备及光电性质研究

采用操作简单的溶胶-凝胶法和射频磁控溅射法在石英衬底上分别制备了MgxZn1-xO薄膜和MgxZn1-xO/Au/MgxZn1-xO夹层结构的透明导电薄膜并对样品进行退火处理。利用紫外-可见分光光度计、X射线衍射仪、光致发光、霍尔效应测试对在不同退火温度下薄膜的晶体结构、光学和电学性质进行表征分析,并研究退火温度对其影响。测试结果表明:所制备的薄膜样品均具有良好的c轴(c-axis)取向并呈现出六角纤锌矿结构。Mg组分的增加使得ZnO基薄膜的光学带隙逐渐增大,PL发光谱和吸收光谱的谱线出现了明显的蓝移现象,但薄膜的电学特性有所降低。而在MgxZn1-xO/Au/MgxZn1-xO夹层结构的薄膜样品中,Au夹层的存在使薄膜的光学性质变差,在紫外区域透光率约为60%。但薄膜的电学性质得到明显改善,相比MgxZn1-xO薄膜,其电阻率和迁移率显著提高。此外通过高温退火处理可以有效提高所制备薄膜的晶体质量,进一步提高样品电学特性,其中经过500℃退火后的薄膜迁移率达到了40.9cm2·Vs-1,电阻率为0.005 7Ω·cm。但随着退火温度的进一步升高,薄膜晶体尺寸从25.1nm增大到32.4nm,从而降低了该薄膜的迁移率。因此该夹层结构的MgxZn1-xO/Au/MgxZn1-xO薄膜对于促进ZnO基透明导电薄膜在深紫外光学器件中的应用有重要作用。     

Mg掺杂ZnO纳米晶的低温共沉淀法制备及光学性质

采用共沉淀(co-precipitation)法制备了Mg掺杂ZnO纳米晶,分别用X射线衍射(XRD)、傅立叶变换红外光谱(FTIR)、紫外可见吸收(UV-Vis)光谱、光致发光(PL)光谱、透射电镜(TEM)、电子顺磁共振(EPR)等分析手段对样品进行了表征。探究了Mg离子在ZnO纳米晶中的存在状态,ZnO纳米晶颗粒尺寸和发射光谱随Mg掺杂浓度的变化,并对其发光机理进行了分析。结果表明:Mg离子在ZnO晶格中以部分晶格位,部分间隙位的方式存在,没有形成MgO表面壳层结构;随Mg掺杂浓度的增大,ZnO纳米晶的颗粒尺寸变小,发射光的光强增大。发射光的最佳激发波长为342nm,中心波长为500nm,荧光量子产率为22.8%。实验分析表明:Mg离子的掺杂在ZnO纳米晶中引入了锌空位(VZn),间隙位的镁离子(IMg),提供了新的复合中心,从而增强了ZnO纳米晶的光致发光。     

Na-Mg共掺杂ZnO薄膜的结构和光学性质

利用溶胶-凝胶法,在普通载玻片上使用旋转涂膜技术制备了具有c轴择优取向生长的Na-Mg共掺杂的ZnO薄膜。用XRD、SEM、光致发光(PL)及透射光谱对薄膜样品进行了表征。结果表明:Na-Mg共掺杂有利于ZnO薄膜的c轴择优取向生长,并且随着Na+掺杂浓度的增加,晶粒尺寸先增大后减小;通过比较不同掺杂浓度ZnO薄膜的PL谱,推测发光峰值位于380nm的紫外发射与ZnO的自由激子复合有关;发现掺入Mg的确能使ZnO禁带宽度增大,掺杂组分为Na0.04Mg0.2Zn0.76O时,其PL谱只有一个很强的紫光发射峰,其近带边紫外光发射强度较未掺杂的ZnO增强了近10倍,极大地提高了薄膜紫外发光性能;并且随Na+浓度增加薄膜透光性减弱。     

MgxZn1-xO薄膜的光致发光性能研究

用溶胶-凝胶旋涂的方法在Si(100)衬底上成功制备了MgxZn1-xO薄膜.通过对样品的X射线衍射花样进行分析,发现制得的样品都有明显的C轴取向.掺入Mg后C轴参数逐渐变小,这表明Mg离子进入了ZnO晶格.随着镁的掺入,其光致发光谱中的紫外发射峰的峰位发生明显蓝移,从3.28eV线性地变化到3.45eV.值得注意的是,掺入镁离子后,薄膜的紫外发光和可见发光的强度都显著高于ZnO.     

Sn掺杂ZnO纳米晶的水热法制备及光学性能

以ZnCl2和NaOH为原料,用SnCl4·4H2O作掺杂剂,通过水热法合成了Sn掺杂ZnO纳米颗粒。利用X射线衍射(XRD)、场发射扫描电镜(FE-SEM)、紫外-可见吸收光谱(UV-Vis)及光致发光(PL)光谱等测试技术对样品的物相、形貌及光学性能进行了表征。结果表明:制得的Sn掺杂ZnO纳米粒子具有六角纤锌矿结构。随着锡掺杂浓度的增大,纳米晶的平均粒度增加,晶体形貌由短棒状向单锥和双锥状转变;提高前驱液的pH值,所得样品的形貌由长柱状向短柱状转变。室温下,观测到三个光致发光带,一个峰值在433nm处的强紫光发射峰,一个约在401nm处的近紫外发光峰及一个在466nm处的弱蓝光发光峰。在实验掺杂浓度范围内,Sn的掺杂只是改变纳米ZnO的发光强度,对发光峰位置影响不大。     

镉掺杂氧化锌纳米花的制备及其光催化活性

以氯化锌、氯化镉、氢氧化钠为原料,采用水热法合成Cd掺杂纳米花状ZnO光催化剂,并通过该样品对罗丹明B水溶液的降解来研究其光催化活性。利用X射线衍射(XRD)、扫描电子显微镜(SEM)、X射线能量色散谱(EDS)、光致发光谱(PL)及紫外-可见分光光度计(UV-Vis)等测试手段对材料物性进行表征。实验结果表明:当掺杂Cd2+时,样品形貌发生变化、粒径减小;掺杂Cd2+后的ZnO的吸收边和紫外峰对比于纯ZnO均发生红移,禁带宽度由3.24 eV减小到3.16 eV。通过光催化实验分析可知,掺杂后纳米ZnO光催化剂对罗丹明B水溶液的降解率有所提高,光照3 h其降解率高达98%,说明与纯ZnO相比,Cd掺杂ZnO纳米花具有更高的光催化活性。     

白宝石衬底上生长的MgxZn1-xO晶体薄膜的结构和光学性能

在白宝石 (sapphire)衬底上低温外延生长出了MgxZn1 -xO晶体薄膜 .x射线衍射 (XRD)及能量色散x射线 (EDX)分析表明 ,MgxZn1 -xO薄膜的晶体结构依赖于薄膜中Mg的组分x,随着Mg组分的增大 ,MgxZn1 -xO薄膜的结构从与ZnO晶体一致的六方结构转变为与MgO晶体一致的立方结构 .对MgxZn1 -xO薄膜的紫外透射光谱及紫外光致荧光谱 (UVPL)的分析表明 ,随着Mg组分的增大 ,光学吸收边产生明显的蓝移 ,表明MgxZn1 -xO晶体薄膜的带隙增大 ,且带隙连续可调 .吸收光谱和XRD测量显示 ,带隙高达 5 6 5eV的MgxZn1 -xO晶体薄膜与MgO之间的晶格失配仅为0 16 % .     

Mg含量对Mg_xZn_(1-x)O∶Ga薄膜电学性质的影响

通过金属有机物化学气相沉积法制备了不同Mg组分的MgxZn1-xO∶Ga(x=0,0.03,0.14)薄膜。透射谱中MgxZn1-xO∶Ga薄膜的光学带隙随x增大而出现的蓝移证实了Mg在Zn O晶格中的替位掺入。薄膜上金叉指电极间的变温I-V曲线显示,在同等温度下,Ga掺杂MgxZn1-xO薄膜的电阻率随着x值的增大而逐渐升高。这是由于Mg组分增大使材料的导带底显著上升,Ga的施主能级深度增大,导致n型载流子浓度降低。根据I-V曲线计算了270 K温度下MgxZn1-xO∶Ga薄膜的浅能级施主深度。与x=0,0.03,0.14对应的施主能级深度分别为45.3,58.5,65 me V,说明随着薄膜Mg含量的升高,Ga的施主能级深度有增加的趋势。     

弯曲纳米光纤的耦合问题研究

从纳米光纤倏逝波角度出发,采用时域有限差分法数值模拟了两根弯曲纳米光纤耦合区域附近的空间光强分布,给出耦合效率随两弯曲光纤间距、光纤半径、弯曲半径等参量变化的曲线.结果表明:两根纳米光纤之间可以有效传递光能,其耦合效率随两弯曲光纤间距、光纤半径、弯曲半径等参量均有关.     

Structural and Optical Properties of Carbon Nanofibers

Technical Physics - Experimental data are reported for bulk globules up to 1 cm3 in volume that consist of 1000-nm-long carbon nanofibers (CNFs) 35–40 nm in diameter. The CNF clews have been...     

Isotope Separation Using Quantum Revival Phenomenon in Nanofibers

We demonstrate the separation of isotopes based on quantum revival phenomenon in nanofibers. We use an optical nanofiber carrying blue-detuned light and red-detuned light. Keeping in view the detuning of atoms with the optical fields, we create attractive and repulsive potentials around the fiber in the radial direction, which produce potential minima in the transverse plane. The wave packets of differing isotopes revive at different quantum revival times and become spatially separated.     

射频等离子体对气相生长碳纳米纤维的氧化改性

"采用不同流量比率的氧气和氩气作为载气,氧化修饰气相生长碳纳米纤维(VGCNFs)．傅立叶红外光谱、热重以及Boehm's滴定法分析结果表明,当氧气含量为4%时,碳纤维表面生成有大量O-H官能团;然而,当氧气含量增加为5%时,在其表面不仅生成有-OH官能团,而且还有-CHx、-CO等官能团出现,说明在适当的氧浓度条件下有利于VGCNFs修饰;但氧气含量继续增加到8%时,其纤维内层石墨晶格氧化断裂,微晶结构被破坏．"     

竹节状纳米碳纤维的制备及嵌锂性能研究

以泡沫镍为催化剂 ,在 6 0 0和 70 0℃下 ,以CVD法热解乙炔气体制备大量的纳米碳纤维 .随着制备温度增加 ,纳米碳纤维直径变小 ,竹节状含量减少 ,d0 0 2 值减小 ,微晶片层平面Lc 和La 值增大 ,碳材料的可逆容量则下降 .分别用透射电镜、X射线衍射和拉曼光谱观察和测定了纳米碳纤维的形貌、微结构 ,发现在不同条件下生长的纳米碳纤维有不同的形貌和结构 .对纳米碳纤维的电化学嵌锂性能的研究表明 ,纳米碳纤维的结构对其电化学嵌锂容量和充放电循环寿命起重要影响 ,制备温度越低 ,纳米碳纤维的石墨化程度越差 ,可逆嵌锂容量相应要高一些     

Sustained Release of Protein Particle Encapsulated in Bead-on-String Electrospun Nanofibers

The feasibility of alleviating burst release of electrospun bead-on-string nanofiber scaffolds loaded with protein particles was evaluated, including an investigation of the influence of the beads number on the release profile. Bovine serum albumin–loaded dextran particles were used as the model drug and poly(lactic-co-glycolic acid) as the polymer to fabricate the bead-on-string nanofiber scaffolds by electrospinning. Both the bead structure and the distribution of the particles in the beads were examined by scanning electron, transmission electron, and fluorescence microscopy. The results of fluorescence microscopy suggested that the particles were well encapsulated by the beads of the fibers. In vitro release tests showed that a more sustainable release profile with less initial burst release could be obtained from the bead-on-string fibers than from smooth fibers with uniform diameter. In addition, when the number of the forming beads was not numerous enough to encapsulate all the particles in the suspensions, the release performance worsened because the surplus particles were not properly encapsulated.     

Production and Characterization of Zirconia (ZrO2) Ceramic Nanofibers by Using Electrospun Poly(Vinyl Alcohol)/Zirconium Acetate Nanofibers as a Precursor

Zirconia (ZrO₂) inorganic ceramic nanofibers were produced using electrospinning of the poly(vinyl alcohol)/zirconium acetate as a precursor followed by calcinating and sintering to decompose the polymer and turn the metal salt (zirconium acetate) into the metal oxide. Characterization of the nanofibers, including polymer thermal decomposition, chemical and crystal structure, phase transformations, and fiber morphology were investigated by simultaneous thermal analysis (STA), thermomechanical analysis (TMA), Fourier transform infrared spectroscopy (FTIR), X-ray diffraction (XRD), and field emission scanning electron microscopy (FESEM). The results showed that the polymer decomposition started at 250°C and zirconia nanofibers with different phases (tetragonal and monoclinic) were obtained by the calcination of the precursor nanofibers at various temperatures between 500°C and 1100°C. The initially crystallized zirconia phase, which formed at 500°C, was tetragonal and with increasing calcination temperature, zirconia nanofibers with increasing amount of monoclinic phase were formed. Consequently, at 1100°C, the tetragonal phase disappeared and was transformed to the monoclinic phase of the zirconia completely. Increasing the calcination temperature caused the fiber average diameter decrease and grain growth took place due to the removal of the polymer and organic groups; neighboring grains sintered to each other and formed fibers with a high aspect ratio. At 1100°C the grains size was about the same as the fiber diameter.     

静电纺丝法制备TiO_2/ZnO复合纳米纤维

利用溶胶—凝胶的方法,将不同量的乙酸锌、钛酸丁酯溶剂及高分子材料混合搅拌,从而获得不同比例的前驱体溶液,然后经过静电纺丝及高温煅烧,获得一维TiO2/ZnO复合纳米纤维,通过扫描电子显微镜对其形貌进行观察,并用XRD确定其组分。