柔性透明石墨烯膜制备及导电性能研究

本文通过液相化学还原和热还原联合作用制备了柔性透明导电石墨烯膜.阳极氧化铝(AAO)模板在制备过程中既作为抽滤的滤网,又作为热还原处理时支撑石墨烯膜的衬底,制成的柔性透明石墨烯膜对波长为540—840 nm的可见光透光率为80%,面电阻为850 Ω/平方,这与化学气相沉积法制备的石墨烯膜(280—770 Ω/平方)相近,而低于溶液法制备的石墨烯膜(通常是10³—10⁴ Ω/平方).     

Controllable synthesis of Ag nanorods using a porous anodic aluminum oxide template

This paper describes a new approach to the synthesis of Ag nanorods. A solvothermal method was used to make Ag nanoparticles inside anodic aluminum oxide (AAO) templates. The nanoparticles were then annealed at 300 °C to produce Ag nanorods. The size of AAO templates, which is focused on in this study, would determine the diameter of Ag nanorods. The product was characterized by X-ray diffraction (XRD), scanning electron microscopy (SEM) and transmission electron microscopy (TEM). In this study, a nanorod growth mechanism is deduced, and understanding of the growth of nanorods inside AAO templates is furthered. This work demonstrates that it is possible to make crystalline nanorods that the size can be varied.     

聚乙烯在氧化铝模板中的结晶与取向行为

用多孔阳极氧化铝(AAO)模板制备了直径为200nm的聚乙烯(PE)纳米纤维,并用傅立叶变换红外光谱(FTIR)、偏光显微镜(PLM)和X-射线衍射(XRD)方法研究了PE在二维圆柱状受限条件下的结晶与取向行为.FTIR研究表明,由于模板的限制作用,PE纳米纤维的结晶度低于本体.同时,PE纳米纤维晶体的b轴平行于模板孔洞的方向取向,而a轴垂直于孔洞的方向取向.XRD结果进一步证明,在纳米孔洞中PE晶体的b轴平行于纳米孔洞方向.PLM结果表明,在结晶过程中,晶体主要是在模板与本体的界面处成核,然后晶体呈发散状向本体和纳米纤维中竞争生长.由于PE晶体的b轴是其生长速率最快的方向,在本体中形成典型的环带球晶形貌;而在二维圆柱受限条件下,只有沿孔洞方向生长的晶体才能增长,而其它生长方向则受到抑制,造成PE晶体的b轴沿孔洞方向优先取向.     

交流电沉积条件对沉积Ni纳米线的影响

采用恒压40V二次阳极氧化方法制备了阳极氧化铝(AAO)模板,模板的孔径均匀有序。在二次阳极氧化的基础上阶梯降低电压至10V,可有效减薄阻隔层,有利于Ni纳米线的交流电沉积。利用扫描电子显微镜和透射电子显微镜对AAO模板以及Ni纳米线的形貌进行表征。探索了阶梯降低氧化电压、电源滤波以及电沉积频率对沉积Ni纳米线的影响。结果表明,阶梯降低氧化电压、适当的频率以及滤波可以明显提高电沉积效果,得到比较均匀有序的Ni纳米线。     

双扩散模板法制备卤化银纳米线及其光催化性能

在室温条件下,通过溶液的双扩散法于AAO模板中制备AgX纳米线,利用XRD,SEM和TEM等分析手段对纳米线进行了表征,结果表明,用该方法合成的AgX纳米线阵列分布均匀,取向性极好,直径50nm,与AAO模板的孔径一致.通过纳米线阵列膜对罗丹明B的降解情况对其光催化活性进行了测试,结果表明AgX纳米线具有良好的光催化性能.     

Growth and optical absorption properties of silver nanorod arrays in porous anodic aluminum oxide templates

Silver nanorod arrays have been fabricated by alternat-ing current(AC) and pulsed direct current(DC) electrodeposition in porous anodic aluminum oxide(AAO) templates with controlled pore diameters of 19,38,and 65 nm,respectively.The variation of their optical absorption properties with the incident angle and the nanorods length(corresponding to the electrodeposition time) has been investigated.Optical absorption spectra show that the posi-tion of longitudinal surface plasmon resonance(LSPR) peak has a small blueshift with the increase of incident angle of the excitation light.While the aspect ratio of the nanorods increases,the position of LSPR peak first redshifts and then blueshifts to a certain wave-length.Furthermore,the position of LSPR peak can be tuned,ranging from 550 nm to 900 nm,which makes it possible to cou-ple various wavelength of excitation source to assist radiative en-ergy transfer to the acceptor.     

量子线器件电致性能模拟研究

用硅基铂钛夹层AAO多孔模板-溶胶凝胶法成功地制备出有序的TiO2纳米线阵列;并用Synopsys TCAD微电子器件仿真软件Sen.Taurus Device模块,模拟分析了单根纳米线的电致物理性能,重点研究纳米线的直径和长度与电导和电压的关系。     

一步法电沉积钯铜二元金属纳米管(英文)

由钯和铜纳米颗粒组成得二元金属纳米管通过电沉积的方法在氧化铝模板中被制备出来.金属离子的扩散和沉积过程的竞争决定了最终的产物是纳米管或者是纳米线.在较高负电位下,其生长受扩散控制,金属离子在纳米管的边缘被消耗,形成的是纳米管结构.而在较低的负电位时形成的是纳米线.在硝酸根离子的电催化实验中,相比于薄膜,纳米管的催化性能受氢气析出的影响较小.在空气中放置6个月后,二元金属纳米管被氧化成均一相的氧化物纳米管.     

磁性氧化铁纳米线的制备与表征

通过溶胶-凝胶法在氧化铝模板（AAO）中制备出了磁性Fe_2O_3纳米线阵列,然后去除AAO模板得到磁性Fe_2O_3纳米线。用SEM,TEM,FTIR,EDX,VSM对磁性纳米线的形貌、微结构和磁性能进行表征。SEM和TEM结果显示磁性纳米线的直径约为50～80nm,长度在8～10μm,长径比为120～180;FTIR和EDX结果表明制备的产物是磁性Fe_2O_3纳米线;VSM结果表明磁性氧化铁纳米线阵列存在明显的磁各向异性。此外,采用Zeta电位仪对磁性Fe_2O_3纳米线表面的电性进行了研究,结果表明纳米线表面带正电荷,有利于和动物细胞相结合。     

Microstructure and magnetic properties of Co-Cu nanowire arrays fabricated by galvanic displacement deposition

CoCu nanowires were fabricated in anodic alumina templates by a simple metal displacement deposition method and the as-deposited samples were subsequently annealed at 400 °C in vacuum. The CoCu nanowires are 80 nm in diameter and 50 μm in length. The aspect ratio (ratio of length to diameter) is larger than 600, which results in distinctive magnetic anisotropy. Enhanced coercivity (about 2245 Oe) and large squareness of 92% have been observed in the annealed samples.