基于LiCo0.8M0.2O2 (M=Ni,Zr)薄膜的全固态薄膜锂电池

用射频磁控溅射结合传统退火的方法制备LiCo0.8M0.2O2 (M=Ni,Zr)阴极薄膜．X射线衍射、拉曼光谱、扫描电子显微镜等手段表征了不同掺杂的LiCo0.8M0.2O2薄膜．结果显示,700℃退火的LiCo0.8M0．2O2薄膜具有类似α-NaFeO2的层状结构．通过对不同掺杂锂钴氧阴极的全固态薄膜锂电池Li／LiPON／LiCo0.8M0.2O2的电化学性能研究表明,电化学活性元素Ni的掺杂使全固态电池具有更大的放电容量(56μAh／cm2μm),而非电化学活性元素Zr的掺杂使全固态电池具有更好的循环稳定性．     

薄膜光学理论与膜系设计

O484.12007010560电沉积-烧结法制备Y2O3∶Eu荧光薄膜的研究=Re-search of luminescence fil m of Y2O3∶Eu prepared bymethod of electrodeposition-sinter[刊,中]/曾冬铭(中南大学化学化工学院.湖南,长沙(410083)),舒万艮…//感光科学与光化学.—2006,24(2).—126-132采用电沉积-烧结方法制备出了氧化钇铕红色荧光薄膜。在0.1mol/L硝酸钇溶液中加入4%(摩尔分数)0.1mol/L硝酸铕掺杂,用三电极体系进行阴极电沉积,工作电极的电位为-1.2V(相对于Ag/AgCl电极),温度65℃,沉积时间为400s,500℃灼烧2h,制备出的发光薄膜与高温固相法制备的…     

沉积温度、膜厚对Ce_(0.8)Gd_(0.2)O_(2-δ)薄膜的微结构和电导率影响

采用脉冲激光沉积法在MgO(100)单晶衬底上制备了Ce0.8Gd0.2O2-δ(CGO)系列薄膜,沉积温度与膜厚对CGO/MgO薄膜的微结构及离子电导率的影响分别被研究.X-ray衍射(2θ-ω线扫描,ω-摇摆曲线,(-扫描)测量显示,随着沉积温度的升高,CGO薄膜的微结构由多晶薄膜演变到外延膜.对沉积在730℃的CGO薄膜(510nm)中较大的离子电导归因于薄膜中较小的晶界密度.对高质外延的CGO薄膜(沉积730℃),随着膜厚的减小,其快速减小的激活能及增大的离子电导可解释为CGO/MgO界面平面的应变态和氧空位的无序分布所致.我们的结果表明,为获得高离子电导的CGO薄膜,最佳的沉积温度和膜厚是需要考虑的.     

氧压对SrTiO3和SrNb0.2Ti0.8O3薄膜晶格参数的影响及激光感生热电电压效应

采用脉冲激光沉积技术制备了SrTiO3和SrNb0.2Ti0.8O3薄膜.X射线衍射分析表明在LaAlO3(100)单晶平衬底上生长的SrTiO3及SrNb0.2Ti0.8O3薄膜是沿[001]取向的近外延生长.随着氧压在一定范围内逐渐增大,SrTiO3薄膜的晶格参数减小,而SrNb0.2Ti0.8O3薄膜的晶格参数先减小后增大.同时摸索出制备具有二维电子气超晶格(SrTiO3/SrNb0.2Ti0.8O3).的最佳氧压为1.0×10-2Pa.另外在LaAlO3(100)倾斜衬底上制备的SrNb0.2Ti0.8O3薄膜中观察到激光感生热电电压效应.     

Ce_(0.8)Pr_(0.2-x)Nd_xO_(2-δ)(x=0.02,0.05,0.1)固溶体的合成与性质研究

采用溶胶-凝胶法制备了双稀土掺杂氧化铈Ce_(0.8)Pr_(0.2-x)Nd_xO_(2-δ)(x=0.02,0.05,0.1)固溶体。X射线衍射分析阐明,经800℃烧结的全部固溶体都形成了单相立方萤石结构,平均晶粒尺寸在20~25 nm之间。拉曼光谱结果阐明,固溶体Ce_(0.8)Pr_(0.2-x)Nd_xO_(2-δ)是具有氧空位的立方萤石结构,适量的掺杂Nd有利于Ce_(0.8)Pr_(0.2-x)Nd_xO_(2-δ)氧空位浓度的增加。阻抗谱结果阐明,稀土双掺杂的Ce_(0.8)Pr_(0.2-x)Nd_xO_(2-δ)比稀土单掺杂的Ce_(0.83)Sm_(0.17)O_(2-y)的电导率高,Ce_(0.8)Pr_(0.18)Nd_(0.02)O_(2-δ)的电导率最大,600℃时电导率为1.85×10~(-2)S/cm。     

氢退火的BZO前电极对非晶硅薄膜太阳能电池性能的影响

采用低压化学气相沉积方法在玻璃衬底上制备了B掺杂的ZnO（BZO）薄膜,通过氢退火对BZO进行处理,然后作为前电极进行了非晶硅薄膜太阳能电池的制备及性能研究。结果表明：在氢气气氛下退火后,BZO薄膜的载流子浓度基本无变化,但Hall迁移率显著提高,这使得BZO薄膜的导电能力提高;当采用厚度较小、透光率较高的BZO薄膜进行氢退火后作为前电极结构时,非晶硅薄膜太阳能电池的短路电流密度提高0.3~0.4 mA/cm²,电池的转化效率提高0.2%。实验结果可为通过优化前电极结构来提高非晶硅薄膜太阳能电池转化效率提供一种简易的方法。     

钙钛矿型中温固体氧化物燃料电池阴极Ba0.5Sr0.5Al0.1Fe0.9O3-δ

研究一种新型不含钴的钙钛矿型中温固体氧化物燃料电池阴极Ba_0.5Sr_0.5Al_0.1Fe_0.9O_3-δ (BSAF)材料的晶体结构、电导率以及在对称电池中的电极极化性能. 研究发现,BSAF阴极在空气中低于450 oC表现出典型的具有正温度系数的半导体行为,最高电导率达到14 S/cm;在450-750 oC,却表现出负温度系数,且电导率在750 oC下降到6 S/cm. 电化学研究表明,在基于混合离子导体的对称电池中,BSAF阴极在650-700 oC表现出良好的电极极化性能.以3%H₂O/H₂为燃料和空气为氧化剂,单电池在700 oC的开路电压和最大功率输出分别达到420 mW/cm².     

(K,Na)NbO_3基无铅压电薄膜的制备与表征（英文）

我们采用脉冲激光沉积法,在SrTiO3(001)衬底上以La0.7Sr0.3MnO3作为底电极,制备得单相的0.95(Na0.49K0.49Li0.02)(Nb0.8Ta0.2)-0.05CaZrO3外延薄膜.采用X射线衍射、X射线光电子能谱,电滞回线和介电常数测试分别表征了LKNNT-CZ薄膜的微观结构、表面元素价态和铁电/介电性能.结果表明:(1)制备得到的LKNNT-CZ薄膜的元素组成与靶材相同;(2)在4伏到10伏内均可以获得线型良好且饱和的电滞回线,当驱动电压为10V时,薄膜的剩余极化达到12.4μC/cm2,矫顽电场为102.3kV/cm;(3)薄膜在1kHz频率下的介电常数高达1185.     

n型InP（100）衬底上电沉积氧化锌薄膜的制备及光致发光

采用电化学沉积方法在n型InP（100）（1016）衬底上制备了氧化锌薄膜。探索线性扫描伏安法确定InP与0．1mol／L Zn（NO3）2电解液的体系中沉积氧化锌的极化电势,在20℃溶液中,相对于甘汞电极（SCE）的极化电势为-1．1877V。扫描电镜照片显示：随着应用电势的降低,氧化锌薄膜变得紧密平滑;狭窄的X射线衍射峰也说明低电势下薄膜的结晶质量较好。光荧光表征发现低电势下制备的氧化锌薄膜具有良好的发光特性。     

电泳沉积法制备V2O5薄膜的结构和性能

将V2O5溶胶电泳沉积在ITO导电基片上制备V2O5薄膜.运用X射线衍射和扫描电镜对薄膜的结构进行分析,通过紫外-可见光透射光谱和循环伏安法分别测试其光学和电化学性能.实验结果表明,电泳沉积V2O5薄膜具有致密的显微结构,薄膜厚度均匀、与基片的粘附性很好;循环实验中,薄膜呈现黄色到绿色的可逆变化,最大的透射率变化达到30%左右;薄膜具有很好的注入/退出可逆性和循环稳定性,50次循环效率仍能达到88.02%,并且循环后的薄膜与ITO导电玻璃的粘附性仍然很好,没有溶解现象;应用交流阻抗法计算Li+在V2O5薄膜着色过程的扩散系数为5.10×10-12cm2/s,表明该薄膜可以作为电致变色材料得到应用.     

凝胶浇注制备La0.8Sr0.2Cr0.5Fe0.5O3-δ-Zr0.84Y0.16O1.92非对称陶瓷透氧膜

要凝胶浇注制备多孔支撑体,并采用浆料涂膜和高温共烧技术制备非对称La_0.8Sr_0.2Cr_0.5Fe_0.5O_3-δ-Zr_0.84Y_0.16O_1.92（LSCF-YSZ）双相复合陶瓷透氧膜。结果显示,采用凝胶浇注制备技术,可获得结构均匀和高孔隙率的多孔支撑体;在多孔支撑体上,采用浆料涂膜和高温共烧技术制备的LSCF-YSZ非对称管状透氧膜,Air/He梯度下,950℃,氧渗透速率达到1.17×10^-8mol·cm^-2·s^-1;在850—950℃温度范围,膜的氧渗透表观活化能为163.7±0.4kJ/mol。     

Promising performances for a La<Subscript>0.6</Subscript>Sr<Subscript>0.4</Subscript>Co<Subscript>0.8</Subscript>Fe<Subscript>0.2</Subscript>O<Subscript>3-δ</Subscript> cathode with a dense interfacial layer at the electrode-electrolyte interface

As for the commonly studied La_0.6Sr_0.4Co_0.2Fe_0.8O_3-δ (6428), here, a very low area-specific resistance (ASR) was measured for La_0.6Sr_0.4Co_0.8Fe_0.2O_3-δ (6482) cathode deposited on a Ce_0.9Gd_0.1O_2-δ (GDC) electrolyte with addition of a thin (1 μm) dense LSCF film deposited by spin coating at the interface between the GDC electrolyte and a 40-μm-thick screen-printed electrode. The ASR ranged from 1 Ω.cm² at 500 °C, 0.11 Ω.cm² at 625 °C and value as low as 0.03 Ω.cm² at 700 °C. Impedance spectra collected in between 500 and 700 °C were carefully studied. They could all be modelled with two R//CPE in series which are likely associated to the oxygen reduction reaction itself (dissociation/adsorption/ionization) at low frequency and to the oxide ion transfer at the electrode/electrolyte interface at high frequency.     

高压下Li掺杂p型ZnO固溶体的表征

报道了利用ZnO和Li₂O混合物在5GPa, 1200 ℃—1500 ℃条件下, 制备Li掺杂p型ZnO(记作ZnO: Li)固溶体的过程. 研究发现, 高压下温度对于ZnO: Li固溶体的导电类型以及结构具有较大的影响. 其中在1500 ℃条件下烧结的ZnO: Li(Li的掺杂量4.5%)表现出良好的p型电学性能, 其电阻率为3.1× 10^-1Ω·cm, 载流子浓度为3.3× 10¹⁹cm^-3, 迁移率为27.7cm²·V^-1·s^-1. 通过实验及理论计算确定了其受主能级为110meV, 讨论了压力对p型ZnO的形成和电学性能的影响.     

Structural,optical and electrical properties of tin oxide thin films by electrostatic spray deposition

Tin oxide (SnO₂) thin films were deposited by electrostatic spray deposition (ESD). The structural, optical and electrical properties of the films for different solvents were studied. The morphology of the deposited thin films was investigated by scanning electron microscopy. The optical transmission spectra of the films showed 66–75% transmittance in the visible region of spectrum. The electrical resistivity of thin films deposited using the different solvents ranged 1.08 × 10^?3–1.34 × 10^?3 Ω-cm. Overall, EG and PG were good solvents for depositing SnO₂ thin films by the ESD technique with stable cone jet.     

TiO2/Al2O3薄膜的原子层沉积和光学性能分析

采用原子层沉积技术在熔石英和BK7玻璃基片上镀制了TiO2/Al2O3薄膜,沉积温度分别为110℃和280℃。利用X射线粉末衍射仪对膜层微观结构进行了分析研究,并在激光损伤平台上进行了抗激光损伤阈值测量。采用Nomarski微分干涉差显微镜和原子力显微镜对激光损伤后的形貌进行了观察分析。结果表明,采用原子层沉积技术镀制的TiO2/Al2O3增透膜的厚度均匀性较好,Φ50 mm样品的膜层厚度均匀性优于99%;光谱增透效果显著,在1 064 nm处的透过率〉99.8%;在熔石英和BK7基片上,TiO2/Al2O3薄膜在110℃时的激光损伤阈值分别为（6.73±0.47）J/cm2和（6.5±0.46）J/cm2,明显高于在280℃时的损伤阈值。     

高温超导YBa2Cu3O7-δ-Y2O3多层薄膜的制备及性能表征

采用脉冲激光沉积技术(PLD)在LaAlO3(100)单晶衬底上外延生长YBa2Cu3O7-δ-Y2O3多层薄膜,用X射线衍射技术(XRD)分析薄膜的物相结构和外延特性,通过原子力显微镜(AFM)观察薄膜的表面形貌.本文主要研究了最佳工艺参数下交替生长多层YBCO-Y2O3膜的超导性能.结果表明,YBa2Cu3O7-δ-Y2O3薄膜为纯c轴取向外延生长,临界电流密度Jc(H=0或H//C)均高于纯YBCO薄膜,纳米Y2O3起到磁通钉扎中心作用.     

Microstructural characterization of La0.4Sr0.6Co0.8Fe0.2O3-δ films deposited by dip coating

The dip-coating method has been successfully used for depositing porous electrodes of La_0.4Sr_0.6Co_0.8Fe_0.2O_3-δ (LSCF) films. Perovskite oxide cobaltites powders have been prepared by an acetic acid-based gel route. Then, cathode films were deposited onto ceramic substrates of the usual electrolyte Cerium Gadolinium Oxide (CGO) by dip coating. The structure and morphology of the powders and films were characterized by X-ray, diffraction (XRD) and scanning electron microscopy (SEM) respectively, to study the correlation between microstructure and deposition parameters. Optimum parameters for obtaining continuous, homogeneous and crack free LSCF films were determined.     

Microstructure and performance of novel Ni anode for hollow fibre solid oxide fuel cells

Nickel anodes were deposited on hollow fibre yttria-stabilised zirconia (YSZ) electrolyte substrates for use in solid oxide fuel cells (SOFCs). The hollow fibres are characterised by porous external and internal surfaces supported by a central gas-tight layer (300 μm total wall thickness and 1.6 mm external diameter). The YSZ hollow fibres were prepared by a phase inversion technique followed by high temperature sintering in the range 1200 to 1400 °C. Ni anodes were deposited on the internal surface by electroless plating involving an initial catalyst deposition step with PdCl₂ followed by Ni plating (with a NiSO₄, NaH₂PO₂ and sodium succinate based solution at 70 °C). Fabrication and nickel deposition parameters (nature of solvents, air gap, temperature, electroless bath composition) and heat treatments in oxidising/reducing environments were investigated in order to improve anode and electrolyte microstructure and fuel cell performance. A parallel study of the effect of YSZ sintering temperature, which influences electrolyte porosity, on electrolyte/anode microstructure was performed on mainly dense discs (2.3 mm thick and 15 mm diameter). Complete cells were tested with both disc and hollow fibre design after a La_0.2Sr_0.8Co_0.8Fe_0.2O_3?δ (LSCF) cathode was deposited by slurry coating and co-fired at 1200 °C. Anodes prepared by Ni electroless plating on YSZ electrolytes (discs and hollow fibres) sintered at lower temperature (1000–1200 °C) benefited from a greater Ni penetration compared to electrolytes sintered at 1400 °C. Further increases in anode porosity and performance were achieved by anode oxidation in air at 1200–1400 °C, followed by reduction in H₂ at 800 °C.     

Spray pyrolytic synthesis of samarium doped ceria (Ce0.8Sm0.2O1.9) films for solid oxide fuel cell applications

Uniform, adherent, single phase samarium doped ceria films have been successfully deposited by spray pyrolysis technique for their application in solid oxide fuel cell. These films have been deposited at different substrate temperatures on glass substrate and subsequently heat treated in tube furnace. Effect of substrate temperature and annealing temperature on phase formation was studied with thermo-gravimetric analysis and differential temperature analysis, X-ray diffraction, scanning electron microscope, and energy dispersive X-ray analysis techniques. These studies showed the formation of single phase Ce_0.8Sm_0.2O_1.9 films, at substrate temperature 400 °C and annealing temperature 550 °C. Electrical resistivity of the films, at room temperature was of the order of 10⁷ Ω cm while at 400 °C it is found to be of the order of 10¹ Ω cm. This reveals the use of these films for making low temperature solid oxide fuel cells.     

原子层沉积制备氧化锌纳米薄膜的光学性质研究

采用原子层沉积技术(ALD),以二乙基锌和水为前驱体,在衬底温度分别为110和190 ℃的条件下制备了致密的氧化锌纳米薄膜。采用X射线光电子能谱,荧光光谱和椭偏仪等表征手段对薄膜的成分和光学性质进行了研究。结果表明,随着沉积温度的增加,氧化锌薄膜内—OH含量降低,说明氧化锌薄膜生长过程中的化学反应更加完全;另外,沉积温度增加后,薄膜在365 nm处的激子发射峰出现了明显的增强,同时可见光区的荧光发射峰消失,表明薄膜内的缺陷态减少。随着成膜质量的提高,氧化锌薄膜的电子迁移率从25提高至32 cm2·(V·S)-1。椭偏测量的拟合结果表明,在375～800 nm的波长范围内,氧化锌薄膜的折射率逐渐从2.33降至1.9,呈现出明显的色散现象;另外,不同温度下制备的氧化锌薄膜光学带隙均为3.27 eV左右,这说明沉积温度对薄膜的带隙没有明显影响。