透明导电ZnO：Sn薄膜光学和电学性能的研究进展

纯ZnO电阻率高,电学性能不稳定,通过掺杂其他元素提高其光电性能,制备出高质量的ZnO薄膜是实现其应用的关键。文章从制备方法、掺杂浓度和退火等方面综述了Sn掺杂ZnO(ZnO:Sn)薄膜光电性能的研究进展,提出了降低ZnO:Sn薄膜电阻率和提高透光率的有效途径。     

微球状ZnO纳米粉体的制备与气敏性能研究

以Zn(CH3COO)2·2H2O为原料,无表面活性剂存在时,利用水热法合成了微球状ZnO纳米粉体。采用XRD,SEM和TEM等测试手段,对其物相、结构进行了表征。结果表明:此粉体为六方晶系的ZnO,结晶良好,直径小于4μm。利用该粉体制成气敏元件,并用静态配气法测试了元件的气敏性能。研究发现:元件在180℃工作温度下,对体积分数为50×10–6的丙酮和乙醇气体的灵敏度分别达到5.9和8.6。     

Al掺杂ZnO薄膜原子力显微图像的多重分形研究

用原子力显微镜观察溶胶-凝胶法制备Al掺杂znO薄膜的表面形貌,运用多重分形理论研究Al掺杂ZnO薄膜的原子力显微图像,多重分形谱可以很好地定量表征薄膜的表面形貌.结果显示:Al掺杂量为0.5 at.%的ZnO薄膜经550℃退火处理后,rms粗糙度为1.817,Al掺杂量为1.0 at.%的ZnO薄膜经600℃退火处理后,rms粗糙度增大到4.625,相应的分形谱宽△α从0.019增大到0.287,分形参数△f由-0.075变为0.124.     

籽晶层退火温度对ZnO纳米棒形貌及发光特性的影响

以不同退火温度处理后的ZnO籽晶层为基底,采用水热法生长了ZnO纳米棒阵列。对制备得到的ZnO纳米棒阵列的形貌、结构以及发光特性进行了表征,分析了籽晶层的退火温度对ZnO纳米棒阵列的形貌及发光性质的影响,发现通过调节籽晶层的退火温度,可以控制ZnO纳米棒的大小及密度,并发现在经400℃退火后的籽晶层上生长的ZnO纳米棒阵列形貌最佳,发光性能最优。     

掺锂氧化锌纳米线的光致发光特性

氧化锌（ZnO）是直接宽带隙半导体材料,有高达60meV的激子束缚能,是下一代短波长光电材料的潜在材料。首先制备了优良的多孔氧化铝（Anodic Aluminum Oxide）有序孔洞阵列;以其为模板,采用直流电化学沉积的方法,在其规则排列的孔中沉积得到锌的纳米线;然后将其在高温下氧化,得到氧化锌的纳米线。XRD图显示Li掺杂前后的ZnO纳米线具有较好的晶态结构。对Li掺杂前后的ZnO纳米线进行光学特性测量,结果表明,ZnO纳米线有两个发光峰,分别位于382nm和508nm处;Li掺杂较大地改善了ZnO纳米线的发光性能,本征发光峰移到395nm处,蓝绿发光强度也有了很大程度的提高。     

立方ZnMgO基体中六方ZnO量子点的化学溶液制备技术

首次报道了利用相分凝技术在非晶石英衬底上立方ZnMgO基体中制备六方ZnO量子点的化学溶液方法.对所制备的ZnO/ZnMgO/SiO2进行了原子力显微镜(AFM)、X射线衍射(XRD)、光致发光(PL)、椭圆偏振光谱(SE)表征.XRD表征表明当六配位Zn2+以替位的形式取代六配位Mg2+时,会导致相同衍射条件下立方ZnMgO的2θ比立方MgO的2θ小.SE表征发现ZnO量子点的量子效应导致了ZnO量子点的激子吸收能(3.76eV)比ZnO体晶的能带隙(3.37 eV)大.AFM表征表明:导致薄膜的XRD的衍射峰、α吸收峰和PL发射峰皆很宽的部分原因是由于组成所制备薄膜的晶粒尺寸分散较大、形状不一引起的.     

Facile deposition of ZnO:Cu films: Structural and optical characterization

Sol–gel technology has been applied for preparation of ZnO:Cu films. The proposed facile approach allows obtaining a wide variety of copper doped zinc oxide systems, revealing different structural and optical behaviors. The work presents structural and optical studies depending on Cu concentration and thermal treatments in the range of 500–800 °C. The structural analysis is performed by X-Ray diffraction (XRD). It reveals that small Cu addition enhances the film crystallization. Increasing copper concentration results in deterioration of ZnO:Cu crystallization. XRD study manifests no Cu oxide phases in ZnO:Cu film structure for lower Cu additions. For a specific higher copper concentration, an appearance of a small fraction of copper oxide is detected. Vibrational properties have been characterized by FTIR spectroscopy. The effect of the copper introduction into ZnO reveals a slight change of optical properties compared to ZnO films for certain Cu ratios. ZnO:Cu films with higher copper contents manifest different optical behaviors with very high transparency in spectral visible range.     

Cu掺杂对ZnO量子点光致发光的影响

通过溶液法合成了Cu掺杂ZnO量子点。X射线衍射(XRD)和高分辨电子透射电镜(HRTEM)图像显示Cu掺杂ZnO量子点具有六角纤锌矿结构,晶粒大小为4～5nm。Cu掺杂抑制了ZnO量子点颗粒长大。室温光致发光(PL)谱观察到紫外带边和可见区两个发射峰。随着Cu掺杂浓度的增大,紫外荧光峰位发生缓慢红移,由366nm移到370nm;可见区发射峰位发生蓝移,由525nm移到495nm;同时,两个发射峰强度降低。光谱结果表明:Cu的掺入,一方面抑制表面与O空位有关的缺陷,在495nm出现了与Cu1+有关的发射峰;另一方面,Cu离子掺入ZnO量子点引入一些非辐射中心,降低了自由激子发射。     

Si基薄膜太阳电池绒面ZGO透明导电膜的研究

采用孪生对靶直流磁控溅射的方法在室温下制备高质量的Ga掺杂ZnO(ZGO)透明导电薄膜,用HCl腐蚀的方法获得满足光散射特性的绒面ZGO薄膜。制备的ZGO样品为具有六角纤锌矿结构的多晶膜,具有(002)方向的择优取向。腐蚀后,绒面ZGO薄膜的晶粒度减小,电阻率基本不变。在可见光范围内,绒面ZGO的反射率比平面ZGO的反射率下降了10%左右。将绒面ZGO薄膜应用于p-i-n型非晶Si薄膜太阳电池中,有效提高了太阳电池性能,使得电池的短路电流提高到17.79 mA/cm2,电池的转换效率增加到7.23%。     

First-principles study of the electronic structures and optical properties of C-F-Be doped wurtzite ZnO

正The electronic structure and optical properties of pure,C-doped,C-F codoped and C-F-Be clusterdoped ZnO with a wurtzite structure were calculated by using the density functional theory with the plane-wave ultrasoft pseudopotentials method.The results indicate that p-type ZnO can be obtained by C incorporation,and the energy level of C_O above the valence band maximum is 0.36 eV.The ionization energy of the complex Zn_(16)O_(14)CF and Zn_(15)BeO_(14)CF can be reduced to 0.23 and 0.21 eV,individually.These results suggest that the defect complex of Zn_(15)BeO_(14)CF is a better candidate for p-type ZnO.To make the optical properties clear,we investigated the imaginary part of the complex dielectric function of undoped and C-F-Be doped ZnO.We found that there is strong absorption in the energy region lower than 2.7 eV for the C-F-Be doped system compared to pure ZnO.