TiO_2/Eu~(3+),Y~(3+)下转换薄膜的制备及其在染料敏化太阳能电池中的应用

采用溶胶-凝胶法制备了TiO2/Eu3+,Y3+下转换薄膜,将其应用到染料敏化太阳能电池中,利用其下转换特性将紫外光转换为可见光,提高了电池的可见光照强度.利用X射线衍射和荧光光谱对TiO2/Eu3+,Y3+粉体进行表征,利用荧光光谱和紫外-可见分光光度计对TiO2/Eu3+,Y3+下转换薄膜进行测试,荧光光谱显示,下转换薄膜受到396nm紫外光照射时可发射出535~620nm连续波长的可见光,具有下转换功能特性.与TiO2薄膜相比,二层下转换薄膜仍能保持较高的可见光透过率.当稀土元素总掺量为4%时,利用下转换特性使短路电流提高了21.5%,光电转换效率提高了14.1%.     

TiO_2/Sm~(3+)下转换薄膜的制备及其在染料敏化太阳能电池中的应用

采用溶胶-凝胶法制备了TiO2/Sm3+下转换薄膜,利用其下转换特性将紫外光转换为可见光,提高了可见光光照强度。利用X射线衍射和荧光光谱对TiO2/Sm3+粉体进行了表征,并对TiO2/Sm3+下转换薄膜进行了荧光光谱测试和紫外-可见分光光度计测试。荧光光谱显示,TiO2/Sm3+薄膜在受到395 nm紫外光照射时可发射出540~600 nm连续波长的可见光,具有下转换特性。二层TiO2/Sm3+下转换薄膜的可见光透过率与单纯的TiO2薄膜基本相同,利用其下转换特性使电池短路电流提高了13.2%,光电转换率提高了16.2%。     

染料敏化太阳能电池Eu~(3+),Sm~(3+)掺杂TiO_2下转换光阳极的制备及性能

用溶胶-凝胶法制备了Eu,Sm共掺TiO_2粉体,将其与P25复合,制备了下转换光阳极,用于染料敏化太阳能电池,利用其下转换特性提高电池的光电性能.用荧光光谱对粉体的发光性能进行表征,荧光光谱显示:Eu,Sm共掺TiO_2粉体受463nm光激发可以发射550~700nm的可见光,具有下转换功能.当Eu~(3+)的摩尔掺杂含量为1%,Sm~(3+)的摩尔含量为0.5%时,制备的Eu~(3+),Sm~(3+)共掺下转换光阳极,短路电流达到14.08mA/cm2,与使用Eu~(3+)掺杂TiO_2的下转换光阳极电池相比,提高了32.08%,转换效率也达到5.29%.     

染料敏化太阳能电池Sm~(3+)掺杂TiO_2下转换光阳极的制备及性能

用溶胶-水热法制备了Sm3+掺杂的Ti O2粉体(Ti O2∶Sm3+),将其按不同质量分数掺杂到P25基体中,制备了具有下转换功能的光阳极,并将其用于染料敏化太阳能电池中,提高了电池的光电性能。荧光光谱显示,Ti O2∶Sm3+粉体可以将紫外光转换为570~700 nm的可见光。当下转换光阳极中Ti O2∶Sm3+粉体的掺杂质量分数为80%时,短路电流密度达到13.12 m A/cm2,与纯P25光阳极相比,提高了26.5%,转换效率也提高了23.5%。     

SrSnO_3∶Sm~(3+)/TiO_2复合光阳极的制备及其光电性能

以Sr(NO_3)_2和NaSnO_3为原料,采用水热法成功制备了SrSnO_3∶Sm~(3+)下转换粉体,并将其与TiO_2复合作为光阳极应用于染料敏化太阳能电池(DSSC)。用X射线衍射仪(XRD)、扫描电子显微镜(SEM)、能谱分析仪(EDS)和荧光光谱仪(FL)对SrSnO_3∶Sm~(3+)进行表征,探讨了SrSnO_3∶Sm~(3+)掺杂量对Sr SnO_3∶Sm~(3+)/TiO_2复合光阳极组装DSSC光电性能的影响。结果表明,通过水热法成功制备了棒状、短柱状和颗粒状混合形貌的SrSnO_3∶Sm~(3+),Sr SnO_3∶Sm~(3+)通过下转换作用将紫外光转换为587 nm的黄色光,拓宽了光谱响应范围。随着SrSnO_3∶Sm~(3+)掺杂量的增加,DSSC的短路电流密度增大。当Sr SnO_3∶Sm~(3+)掺杂质量分数为3%时,短路电流密度和光电转换效率分别为10.3 m A/cm2和4.09%,与纯P25相比,分别提高了38%和25%。     

二甲基亚砜添加剂对聚合物太阳能电池性能的影响

研究了二甲基亚砜(DMSO)掺杂浓度对基于聚(3-己基噻吩)(P3HT)和(6,6)-苯基碳60丁酸甲酯(PCBM)为有源层的聚合物太阳能电池性能影响。结果表明,掺杂DMSO可以提高聚合物太阳能电池短路电流密度和填充因子。DMSO掺杂质量比为3%时,电池短路电流密度提高到7.88 mA·cm-2,填充因子为55.5%。能量转换效率达到2.54％,相比没有掺杂DMSO的电池,能量转换效率提高了17%。傅里叶变换红外光谱被用于鉴定和分析掺杂DMSO对材料P3HT∶PCBM化学性质的影响。傅里叶变换红外光谱表明,掺杂后P3HT和PCBM的化学性质都没有改变。为分析掺杂DMSO改善器件能量转换效率的原因,通过紫外-可见光谱和电流密度-电压特性曲线分别表征器件的光吸收能力以及电致发光器件的载流子迁移率。与P3HT∶PCBM薄膜相比,P3HT∶PCBM∶DMSO薄膜在可见光范围内的吸收峰有明显红移且吸收强度增强。可见光吸收的改善是实现短路电流密度提高的有力保障。太阳能电池性能的增强是因为DMSO的掺杂提高了P3HT∶PCBM的载流子迁移率和吸收光谱宽度。     

二甲基亚砜添加剂对聚合物太阳能电池性能的影响（英文）

研究了二甲基亚砜(DMSO)掺杂浓度对基于聚(3-己基噻吩)(P3HT)和(6,6)-苯基碳60丁酸甲酯(PCBM)为有源层的聚合物太阳能电池性能影响。结果表明,掺杂DMSO可以提高聚合物太阳能电池短路电流密度和填充因子。DMSO掺杂质量比为3%时,电池短路电流密度提高到7.88mA·cm-2,填充因子为55.5%。能量转换效率达到2.54%,相比没有掺杂DMSO的电池,能量转换效率提高了17%。傅里叶变换红外光谱被用于鉴定和分析掺杂DMSO对材料P3HT∶PCBM化学性质的影响。傅里叶变换红外光谱表明,掺杂后P3HT和PCBM的化学性质都没有改变。为分析掺杂DMSO改善器件能量转换效率的原因,通过紫外-可见光谱和电流密度-电压特性曲线分别表征器件的光吸收能力以及电致发光器件的载流子迁移率。与P3HT∶PCBM薄膜相比,P3HT∶PCBM∶DMSO薄膜在可见光范围内的吸收峰有明显红移且吸收强度增强。可见光吸收的改善是实现短路电流密度提高的有力保障。太阳能电池性能的增强是因为DMSO的掺杂提高了P3HT∶PCBM的载流子迁移率和吸收光谱宽度。     

ZnO∶(Al,Sm)阻挡层薄膜的制备及其光电性能

采用溶胶凝胶法制备ZnO∶Al,Sm阻挡层薄膜,并用X射线衍射仪(XRD)、能谱仪(EDS)、红外光谱(FTIR)、荧光光谱(PL)、紫外可见光谱(UV-Vis)和扫描电子显微镜(SEM)等对阻挡层薄膜进行了表征,探讨了Al、Sm掺杂量对阻挡层薄膜性能的影响。结果表明:当Al的掺杂摩尔分数为1%、Sm的掺杂摩尔分数为3%时,所制备的阻挡层荧光强度最高,可将部分紫外光下转换为588nm的可见光,拓宽了光谱响应范围;基于ZnO∶1%Al,3%Sm阻挡层的海胆棘壳色素敏化的纳米TiO_2太阳能电池的开路电压为0.73V,短路电流密度为0.68mA/cm~2,转换效率达0.33%,效率比基于ZnO阻挡层的电池提高了约136%。     

缓冲夹层影响异质结有机光伏器件性能研究

制备了结构为CuPc/缓冲层/C60异质结的有机光伏器件,分别选用三氧化钼和红荧烯为缓冲层,研究了增加缓冲层对器件性能的影响.结果表明,增加三氧化钼和红荧烯缓冲层后器件的开路电压和光电转换效率都得到提高,器件的短路电流密度和填充因子都有所降低.开路电压从没有缓冲层时的0.39V分别提高到0.58V、0.55V,转换效率从0.36%提高到0.44%,短路电流从1.92mA/cm2分别降低到1.77mA/cm2、1.81mA/cm2,填充因子从0.48分别减少到0.43、0.44.进一步研究表明器件的短路电流密度受缓冲层厚度的影响很大,当缓冲层厚度很小时,器件短路电流密度还有所增加,但随着缓冲层厚度的增加,短路电流密度逐渐减小,当缓冲层厚度为10nm时,器件短路电流密度减少到0.35mA/cm2.开路电压随着厚度的增加逐渐增加,从1nm时的0.43V增加10nm时0.63V.根据整数电荷转移模型和界面能级理论解释有机光伏器件开路电压提高以及短路电流密度减少的原因,为有机太阳能电池性能的改善提供了研究方法.     

染料掺杂聚合物薄膜的光谱下转换研究

在玻璃基片表面制作了Coumarin 500、Coumarin 540和Rhodamine 6G 3种染料掺杂的聚合物薄膜,并以市售LED灯和氙灯为光源,实验研究了单一染料掺杂和混合染料掺杂的聚合物薄膜的吸收光谱、荧光光谱及其光谱下转换的特征。研究结果表明：这种多染料掺杂的聚合物薄膜能够吸收350~550 nm波长范围内的光子并将其转换至波长为580 nm左右的光子。在一定的浓度范围内,较高的染料浓度能够获得较高的下转换光子输出。由于Nd³⁺/Yb³⁺共掺玻璃中Nd³⁺离子在 580 nm 附近有一个较强的吸收峰,这种染料掺杂聚合物薄膜的光谱下转换有助于提高Nd³⁺/Yb³⁺共掺玻璃对太阳光中蓝绿光的吸收并通过共振能量转移激发Yb³⁺离子的近红外发光,对提高单晶硅太阳能电池的综合光伏转换效率有潜在的应用价值。     

Optical spectroscopy of Ca3Sc2Si3O12, Ca3Y2Si3O12 and Ca3Lu2Si3O12 doped with Pr

The silicates Ca₃Sc₂Si₃O₁₂, Ca₃Y₂Si₃O₁₂ and Ca₃Lu₂Si₃O₁₂, both undoped and doped with Pr³⁺ ions, have been synthesized by solid-state reaction at high temperature. The luminescence spectroscopy and the excited state dynamics of the materials have been studied upon VUV and X-ray excitation using synchrotron radiation. All doped samples have shown efficient 5d-4f emission upon direct VUV excitation of 5d levels, but only Ca₃Sc₂Si₃O₁₂:Pr³⁺ shows luminescence upon interband VUV or X-ray excitation. The VUV excited emission spectra of Ca₃Y₂Si₃O₁₂:Pr³⁺ and Ca₃Lu₂Si₃O₁₂:Pr³⁺ show features attributed to emission from two distinct sites accommodating the Pr³⁺ dopant. The decay kinetics of the Pr³⁺ 5d-4f emission in Ca₃Sc₂Si₃O₁₂:Pr³⁺ upon VUV excitation across the band gap are characterized by decay times in the range 25-28 ns with no significant rise after the excitation pulse. They appear to be faster upon X-ray irradiation than for VUV excitation. Weak afterglow components are attributed to defect luminescence.     

Multilayer Bi1.5Zn1.0Nb1.5O7/Ba0.6Sr0.4TiO3/Bi1.5Zn1.0Nb1.5O7 thin films for tunable microwave applications

Bi_1.5Zn_1.0Nb_1.5O₇/Ba_0.6Sr_0.4TiO₃/Bi_1.5Zn_1.0Nb_1.5O₇ tunable multilayer thin film has been fabricated by pulsed laser ablation and characterized. Phase composition and microstructure of multilayer films were characterized by X-ray diffraction, scanning electron microscopy (SEM) and atomic force microscopy (AFM). The film has very smooth surface with RMS roughness of 1.5-2 nm and grain size of 100-150 nm. Total film thickness has been measure to be 375 nm. The BZN thin films at 300 K, on Pt(1 1 1)/SiO₂/Si substrate showed zero-field dielectric constant of 105 and dielectric loss tangent of 0.002 at frequency of 0.1 MHz. Thin films annealed at 700 °C shows the dielectric tunability of 18% with biasing field 500 kV/cm at 0.1 MHz. The multilayer thin film shows nonferroelectric behavior at room temperature. The good physical and electrical properties of multilayer thin films make them promising candidate for tunable microwave device applications.     

La0.67Ca0.33MnO3薄膜皮秒光电效应

在1064 nm波长脉冲激光（脉宽25 ps）的照射下，钙钛矿氧化物薄膜La0.67Ca0.33MnO3/SrTiO3具有超快光电效应，对激光脉冲显示ps量级的响应时间，上升沿响应时间300 ps，半高宽700 ps，同时，对激光能量的响应灵敏度为500 mV/mJ。     

合成反铁磁Ni81Fe19/Co90Fe10/Ru/Co90Fe10/Ni81Fe19的研究

采用直流磁控溅射方法制备了一系列的合成反铁磁及以其为自由层的自旋阀.研究发现,在Ni₈₁Fe₁₉与Ru层之间插入适当厚度的Co₉₀Fe₁₀层后,可有效地提高合成反铁磁两磁性层间的反铁磁耦合强度,得到具有饱和场H_s更高、饱和磁化强度M_s更低、热稳定性更好的合成反铁磁.另外,以这种合成反铁磁作自旋阀的自由层时,可有效提高自旋阀的稳定性. 关键词： 合成反铁磁 退火 自旋阀     

Structure and magnetic order in La0.7Ca0.3Mn0.5Co0.5O3 and La0.8Sr0.2Mn0.5Co0.5O3 perovskites

In this paper we report the study of the perovskites La_0.7Ca_0.3Mn_0.5Co_0.5O₃ and La_0.8Sr_0.2Mn_0.5Co_0.5O₃ by neutron powder diffraction at various temperatures and magnetization measurements in zero applied field and at low cooling regimes. The replacement of half Mn by Co in La_0.7Ca_0.3MnO₃ and La_0.8Sr_0.2MnO₃ destroys their long-range ferromagnetism exhibiting a cluster glass ferromagnetic order similar to the one observed in many cobaltites.     

Depolarization currents in the Na0.5Bi8.5Ti2Nb4O27 and Na0.5Bi8.5Ti2Ta4O27 layered ferroelectrics

The influence of the prehistory on the electrical properties of layered ferroelectrics is investigated. It is established that the heating of short-circuited samples of the nonpolarized ceramic material Na_0.5Bi_8.5Ti₂Nb₄O₂₇ leads to the appearance of maxima of the current at temperatures below the Curie point only in the case of preliminary ageing of the samples. Original Russian Text ? A.I. Burkhanov, Yu.V. Kochergin, K. Bormanis, A. Kalvane, M. Dambekalne, 2009, published in Fizika Tverdogo Tela, 2009, Vol. 51, No. 7, pp. 1393–1394.     

Phase formation and characterization of Sr3Y2Ge3O12, Sr3In2Ge3O12, and Ca3Ga2Ge3O12 doped by trivalent europium

This work reports on the phase formation during a solid-state reaction of Eu³⁺-doped garnets with the general formula A₃B₂Ge₃O₁₂ (A=Ca, Sr and B=Ga, In, Y) and their luminescent properties. It is shown by XRD and DTA/TG experiments that the garnet-phase formation is completed at 1100-1200 °C. Moreover, it turned out that the position of the oxygen to europium charge-transfer band and the intensity of the forbidden 4f-4f transitions of Eu³⁺ is dependent on the covalent interaction between the Eu³⁺ activator and the surrounding oxygen anions. The investigated red-emitting luminescent materials show high lumen equivalents and deep red emission at the same time, which makes them attractive for the application in LEDs (light emitting diodes), in particular for near UV-emitting LEDs.     

Appearance of an inhomogeneous superconducting state in La0.67Sr0.33MnO3-YBa2Cu3O7-La0.67Sr0.33MnO3 trilayers

An experimental study of proximity effect in La_0.67Sr_0.33MnO₃-YBa₂CU₃O₇-La_0.67Sr_0.33MnO₃ trilayers is reported. Transport measurements on these samples show clear oscillations in critical current (I _c) as the thickness of La_0.67Sr_0.33MnO₃ layers (d _F) is scanned from ∼50 ? to ∼ 1100 ?. In the light of existing theories of ferromagnet-superconductor (FM-SC) heterostructures, this observation suggests a long range proximity effect in the manganite, modulated by its weak exchange energy (∼2 meV). The observed modulation of the magnetic coupling between the ferromagnetic LSMO layers as a function of d _F, also suggests an oscillatory behavior of the SC order parameter near the FM-SC interface.      

X-ray study of phase transitions in the system of solid solutions K2Pb4Nb10O30-Na2Pb4Nb10O30-K6W4Nb6O30

Boundaries of morphotropic phase transitions region in the system of solid solutions K₂Pb₄Nb₁₀O₃₀-Na₂Pb₄Nb₁₀O₃₀-K₆W₄Nb₆O₃₀ with the structure of the tetragonal tungsten bronze have been specified. Presence of the second morphotropic phase transition, perpendicular to the first one has been revealed. The temperature dependences of the structural parameters of some compounds have been investigated. The compounds with high values of Curie temperatures and working temperatures have been obtained.     

Incommensurate modulations in Ba2TiSi2O8, Sr2TiSi2O8, and Ba2TiGe2O8

Incommensurate modulations in Ba₂TiSi₂O₈, Sr₂TiSi₂O₈, and Ba₂TiGe₂O₈ are compared based on their corresponding electron diffraction patterns. The dependence of the modulations on chemical composition provides a suitable model system for the investigation of incommensurations in framework structures using high-resolution transmission electron microscopy (HRTEM). A widening of quantitative HRTEM utilising the concept of rigid units is proposed allowing for a determination of atomistic displacements responsible for the formation of incommensurately modulated structures.