不同衬底沉积Ti-Al共掺杂ZnO薄膜的性能对比研究

利用直流磁控溅射法,在玻璃衬底和Si片衬底上分别沉积出了Ti-Al共掺杂ZnO透明导电薄膜(TAZO),并对这两种衬底上的薄膜的应力、结构和光电性能进行了对比研究.结果表明:玻璃衬底和Si片衬底上沉积的TAZO薄膜均为具有c轴择优取向的六角纤锌矿结构多晶薄膜,Si片衬底的TAZO薄膜的导电性能优于玻璃衬底上的TAZO薄...     

Al-Zr共掺杂ZnO透明导电薄膜制备及光电性能研究

采用直流磁控溅射法,在室温水冷玻璃衬底上制备出Al-Zr共掺杂的ZnO透明导电薄膜。研究结果表明,Ar气压强对Al-Zr共掺杂ZnO透明导电薄膜的结构和电阻率有显著影响。X射线衍射(XRD)表明,Al-Zr共掺杂ZnO透明导电薄膜为六角纤锌矿结构的多晶薄膜,且具有C轴择优取向。扫描电镜(SEM)观察表明,Ar气压强对Al-Zr共掺杂ZnO透明导电薄膜的微观结构影响较大。薄膜的厚度随Ar气压强的增加而变薄,在Ar气压强为2.5Pa时,制备的Al-Zr共掺杂ZnO薄膜电阻率具有最小值1.01×10-3Ω.cm,在可见光区(500～800nm)平均透过率超过93%。     

低温制备Mn-W共掺ZnO透明导电薄膜

利用直流磁控溅射法成功地在室温玻璃衬底上制备出了电阻率低、透光率高的Mn-W共掺ZnO（ZMWO）透明导电薄膜。溅射功率在65-150 W之间变化。实验结果表明,溅射功率对ZMWO薄膜的晶化程度和电阻率有很大影响,而对其透光率和光学带隙影响不大。实验制备的ZMWO为六方纤锌矿结构的多晶薄膜,具有垂直于衬底方向的c轴择优取向。考虑到薄膜的电学、光学性能及结晶质量,我们认为本实验中的最佳值溅射功率为90 W,在此功率下制备的ZMWO薄膜的电阻率具有最小值9.8×10-4Ωcm,其可见光透过率为89%。     

溅射功率对Zr,Al共掺杂ZnO薄膜结构和性能的影响

室温下,采用直流磁控溅射法,在载玻片衬底上制备出了Zr,Al共掺杂ZnO(AZZO)透明导电薄膜。研究了溅射功率对薄膜的组织结构、表面形貌和光电学性能的影响。结果表明,制备的AZZO透明导电薄膜为六角纤锌矿结构的多晶薄膜,且具有c轴择优取向。当溅射功率为150W时,薄膜电阻率达到最小值1.66×10–3Ω·cm,在可见光区平均透过率超过93%。     

铝钛共掺杂氧化锌透明导电薄膜的制备与性能研究

用直流磁控溅射法在玻璃衬底上成功制备出了铝钛共掺杂氧化锌(TAZO)透明导电薄膜,研究了溅射压强对TAZO薄膜的微观结构和光电特性的影响。研究结果表明,所制备的TAZO薄膜为六角纤锌矿结构的多晶薄膜,且具有c轴择优取向。当溅射压强为7.5Pa时,薄膜的最小电阻率为3.34×10-4Ω.cm。薄膜的可见光区平均透过率大于89%。溅射压强对薄膜的电阻率和微观结构有显著影响。     

ZnO∶Ti透明导电薄膜的制备与光电性能研究

采用直流磁控溅射法,在水冷7059玻璃衬底上制备了具有高透射率和相对低电阻率的掺钛氧化锌(ZnO∶Ti)透明导电薄膜,研究了溅射偏压对ZnO∶Ti薄膜结构、形貌和光电性能的影响。结果表明,ZnO∶Ti薄膜为六角纤锌矿多晶结构,具有c轴择优取向。溅射偏压对ZnO∶Ti薄膜的结构和电阻率有重要影响。当溅射偏压为10V时,电阻率具有最小值1.90×10–4?.cm。薄膜具有良好的附着性能,可见光区平均透射率超过90%。该ZnO∶Ti薄膜可以用作薄膜太阳能电池和液晶显示器的透明电极。     

ZnO:Ti透明导电薄膜的制备与光电性能研究

采用直流磁控溅射法,在水冷7059玻璃衬底上制备了具有高透射率和相对低电阻率的掺钛氧化锌(ZnO:Ti)透明导电薄膜,研究了溅射偏压对ZnO:Ti 薄膜结构、形貌和光电性能的影响.结果表明,ZnO:Ti 薄膜为六角纤锌矿多晶结构,具有c轴择优取向.溅射偏压对ZnO:Ti 薄膜的结构和电阻率有重要影响.当溅射偏压为10 V时,电阻率具有最小值1.90×10–4 Ω· cm.薄膜具有良好的附着性能,可见光区平均透射率超过90%.该ZnO:Ti薄膜可以用作薄膜太阳能电池和液晶显示器的透明电极.     

In掺杂ZnO透明导电薄膜光电性质的研究

采用射频磁控溅射技术成功制备出无掺杂和In掺杂的ZnO透明导电薄膜.研究了In掺杂对薄膜的结构和光电性能的影响.结果表明,In掺杂有利于提高ZnO薄膜结晶度,使薄膜表面更加致密平整;由于In3+替代了Zn2+,提供了大量的剩余电子,使薄膜的导电性质得到了很大的提高,所得薄膜的最小电阻率为4.3×10-3Q·cm.制备的ZnO薄膜在可见光范围的透过率达到了85%,In的掺杂对透光率的影响不大.     

沉积时间对Sn-Mg共掺ZnO薄膜光电性能的影响

采用超声喷雾热解法在石英玻璃衬底上,在衬底 温度为440 ℃,喷嘴到衬底距离为4cm,掺杂原子(Zn∶Mg∶Sn)比例为97.6∶2∶0.4,载气流量为0.8 L/min的固定条件下,制备了不同薄膜沉积时间(5min、 7min、9min、11 min)的Sn-Mg共掺的ZnO薄膜。并用X射线衍射仪 (XRD)、扫描电子显微镜(SEM)、 光致发光谱(PL)、紫外可见分光光度计(UV-VIS)、薄膜测厚仪(SCG-10)和伏安特性曲线(I-V)对 薄膜的结构、表面形貌、发光性能、透过率、膜厚和电学性能进行了一系列表征。当沉积时 间为7min时, XRD表明,薄膜的(101)峰强度最大,择优取向明显。SEM图显示薄 膜表面致密光滑,颗粒均匀,尺寸 最大且形貌最佳。PL谱在372 nm处的发射峰强度最大,峰形最尖锐, 所有薄膜的透过率在可见光区域都 超过了80%,表现出了很好的光透过性能。从薄膜的I- V特性曲线可计算出此时的电阻最小,导电性能最佳。     

(Al,Zr)共掺杂ZnO透明导电薄膜的结构以及光电性能研究

用射频磁控溅射法在玻璃衬底上氩气气氛中制备出(Al,Zr)共掺杂的ZnO透明导电薄膜,研究了不同Zr掺杂浓度和薄膜厚度ZnO薄膜的结构、电学和光学特性。结果表明,在最佳沉积条件下我们制备出了具有(002)单一择优取向的多晶六角纤锌矿结构,电阻率为2.2×10-2Ω.cm,且可见光段(320～800nm)平均透过率达到85%的ZnO透明导电薄膜。在150℃的条件下对(Al,Zr)共掺杂的ZnO薄膜进行1h的退火处理,薄膜电阻率降低至8.4×10-3Ω.cm。Zr杂质的掺入改善了薄膜的可见光透光性。     

低电阻率高透过率TAZO透明导电膜的制备及性能

利用直流磁控溅射工艺,在水冷玻璃衬底上制备了透过率高、电阻率相对较低的钛铝共掺杂ZnO(TAZO)透明导电膜。用XRD和SEM等研究其结构、应力和光电性能与靶基距之间的关系。结果表明:TAZO薄膜为六方纤锌矿结构的多晶薄膜,且具有c轴择优取向。当靶基距为42mm时,薄膜样品晶格畸变最小,具有最小压应力(绝对值)0.270GPa,同时具有最小方块电阻4.21?/□;靶基距为48mm时,薄膜样品具有最小电阻率3.09×10–4?·cm。所有薄膜样品的可见光区平均透过率都超过了91%。     

Low-temperature deposition of transparent conducting Mn-W co-doped ZnO thin films

Mn-W co-doped ZnO(ZMWO) thin films with low resistivity and high transparency were successfully prepared on glass substrate by direct current(DC) magnetron sputtering at low temperature.The sputtering power was varied from 65 to 150 W.The crystallinity and resistivity of ZMWO films greatly depend on sputtering power while the optical transmittance and optical band gap are not sensitive to sputtering power.All the deposited films are polycrystalline with a hexagonal structure and have a preferred orientat...     

Influence of the distance between target and substrate on the properties of transparent conducting Al-Zr co-doped zinc oxide thin films

Highly transparent and conducting AI-Zr co-doped zinc oxide (ZAZO) thin films were successfully prepared on glass substrate by direct current (DC) magnetron sputtering at room temperature. The distance between target and substrate was varied from 45 to 70 mm. All the deposited films are polycrystalline with a hexagonal structure and have a preferred orientation along the c-axis perpendicular to the substrate. The crystallinity increases obviously and the electrical resistivity decreases when the distance between target and substrate decreases from 70 to 50 mm. However, as the distance decreases further, the crystallinity decreases and the electrical resistivity increases. When the distance between target and substrate is 50 mm, it is found that the lowest resistivity is 6.9×10~(-4) Ω·cm.All the deposited films show a high average transmittance of above 92% in the visible range.     

Influence of the distance between target and substrate on the properties of transparent conducting AI-Zr co-doped zinc oxide thin films

Highly transparent and conducting Al-Zr co-doped zinc oxide （ZAZO） thin films were successfully prepared on glass substrate by direct current （DC） magnetron sputtering at room temperature. The distance between target and substrate was varied from 45 to 70 mm. All the deposited films are polycrystalline with a hexagonal structure and have a preferred orientation along the c-axis perpendicular to the substrate. The crystallinity increases obviously and the electrical resistivity decreases when the distance between target and substrate decreases from 70 to 50 mm. However, as the distance decreases further, the crystallinity decreases and the electrical resistivity increases. When the distance between target and substrate is 50 ram, it is found that the lowest resistivity is 6.9 × 10^-4Ω cm. All the deposited films show a high average transmittance of above 92% in the visible range.     

Influence of the distance between target and substrate on the properties of transparent conducting Al-Zr co-doped zinc oxide thin films

Highly transparent and conducting Al-Zr co-doped zinc oxide (ZAZO) thin films were successfully prepared on glass substrate by direct current (DC) magnetron sputtering at room temperature.The distance between target and substrate was varied from 45 to 70 mm.All the deposited films are polycrystalline with a hexagonal structure and have a preferred orientation along the c-axis perpendicular to the substrate.The crystallinity increases obviously and the electrical resistivity decreases when the distance betwe...     

透明导电薄膜ZnO:Zr的反应磁控溅射法制备及表征

以Zn金属靶和Zr金属片组成的Zn:Zr为靶材,利用直流反应磁控溅射法在玻璃衬底上制备ZnO:Zr透明导电薄膜。研究了靶与衬底之间的距离对所制备薄膜结构和性能的影响。实验制备的ZnO:Zr薄膜为六方纤锌矿结构的多晶薄膜,且具有与衬底方向垂直的c轴择优取向。实验结果表明,靶与衬底之间的距离对ZnO:Zr薄膜的结构、生长速率、密度及电学性能有很大影响。靶与衬底之间的最佳距离为6.0cm,在此条件下制备的ZnO:Zr薄膜具有最小电阻率1.78×10-3Ω.cm,其可见光透过率为88.5%,折射率为2.04。     

NZO透明导电薄膜的制备及其性能研究

室温下,采用直流磁控溅射法,在玻璃衬底上制备出Nb掺杂ZnO(NZO,ZnO:Nb)透明导电薄膜。研究了靶与衬底之间的距离对NZO薄膜结构、形貌、光学及电学性能的影响。实验结果表明,不同靶基距下制备的NZO薄膜均为c轴择优取向生长,(002)衍射峰的强度随着靶基距的减小而增大。靶基距增大时,薄膜表面逐步趋向平整光滑、均匀致密,薄膜的厚度逐渐减小。在靶基距为60mm时,制备的薄膜厚为355.4nm,电阻率具有最小值(6.04×10-4Ω.cm),在可见光区的平均透过率达到92.5%,其光学带隙为3.39eV。