Cu_xC_(60)薄膜紫外-可见吸收光谱研究

近来,有关 C60的研究主要集中在有关晶格动力学 [1]、电子结构 [2～ 4]和 MxC60（ M代表碱金属或碱土金属）的超导电性研究 [5].但由于 MxC60在大气中不能稳定存在,制约了 MxC60的深入研究和实际应用 .最近, Masterov等人报导了他们对 Cu/C60的超导特性研究 [6～ 7],认为其转变温度 Tc在 80～ 120 K之间,这个转变温度比现有的 MxC60的转变温度（ Tc～ 40 K）要高得多 .但有关更进一步的研究未见报导 .因此,我们拟对 CuxC60体系作较为详尽的研究,这对于进一步研究其超导机理是有必要的 .本工作是在成功地制备了 CuxC60薄膜的…     

晶态Ca3C60与Ca5C60的能带结构研究

用三维EHMO晶体轨道程序分别对Ca3C60，Ca5C60进行了能带结构的计算．计算结果表明，Ca3C60没有导电性，能隙约为0．9eV；而在Ca5C60的能带结构中，费米面刚好穿过半满带，表明Ca5C60是导体；同时在费米面附近有较大的态密度值，表明Ca5C60与K3C60等类似，具有较高的超导转变温度．电荷分析表明，在这两种情况下，钙原子的4s电子基本上全转移到C60上，C60分子可形成一个稳定的带6到10个电子的负离子．     

CSD法超导薄膜的形成机制和超导电性研究

利用化学喷雾沉积法（CSD法）在未定向的ZrO2单晶衬底上获得了零电阻温度高于85K和转变宽度为2K、厚度小于5μm的YBa2Cu3O7-δ超导薄膜，以XRD、XPS和SEM等手段研究了不同制备条件下薄膜的晶体结构、电子结构和显微表貌，讨论了材料膜形成机制及其与超导电性的关系。     

La1.8Sr0.2CuO4/La1.9Sr0.1CuO4超导双层薄膜的制备及电学输运性能研究

采用Nd:YAG固体激光器在SrTiO3(STO)衬底上成功制备了具有c轴取向的过掺杂La1.8Sr0.2CuO4和欠掺杂La1.9Sr0.1CuO4超导薄膜。分别对薄膜的晶体结构、电学输运性能进行了研究。通过晶体结构分析表明超导薄膜沿<001>晶向生长,沉积后的薄膜超导转变温度(TC)随着薄膜厚度(20～200 nm)的增加而逐渐升高,显示薄膜由二维特征向三维特征过渡。在双层薄膜La1.8Sr0.2CuO4/La1.9Sr0.1CuO4结构中,其电学输运性能和所加电场的方向有很大关联,反映出电场的方向影响了超导薄膜中空穴载流子的扩散,进而影响了薄膜的超导转变温度和电学输运性能。     

合成气制低碳烯烃用Fe／AC催化剂的制备及性能表征

 研究了以活性炭（AC）作为载体制备的铁基催化剂，通过对不同铁盐、活性炭和助剂的筛选，研制出对合成气转化为低碳烯烃具有高活性和高选择性的催化剂．对反应前及反应过程中催化剂体相结构的XRD测试结果表明，Fe－Cu－K／AC催化剂在反应前主要由α－Fe，Fe3O4和Cu0组成，经合成气反应后主要由α－Fe，Fe5C2，Fe7C3，Cu0和K2O组成．Fe－Mn－K／AC催化剂的晶体结构主要以Fe嵌入MnO中形成的（Fe，Mn）O结构存在．实验中得出的α－Fe，FexCy及（Fe，Mn）O与激光热解法制备的催化剂的的晶体结构相似．对催化剂的制备方法进行了筛选，考察了不同助剂Cu，Mn，Si和K等元素对催化剂性能的影响．结果表明，以草酸铁为铁源，椰壳炭为载体制备的Fe－Mn－K／AC催化剂的催化效果最佳，在空速600h－1，压力1．5MPa和温度320℃条件下，CO转化率可达97．4％，C＝2～C＝4选择性可达68．0％．     

高温超导材料的表界面化学研究

超导现象早在1911年就为世人所知. 基于超导材料和超导技术广阔的应用前景, 一百多年来来自物理、化学、材料等不同领域的研究者们一直为发现新的、高超导转变温度(甚至室温)的超导材料而不断努力. 同时, 超导材料的表界面研究工作也越来越受到关注. 本文首先介绍了过去国内外研究者在铜基氧化物超导材料表面的一些分子吸附研究工作, 随后总结了最近在超导薄膜体系中界面效应对提高超导转变温度及其研究超导机制的意义, 着重揭示了表面/界面在超导研究和发展中的重要性.     

新型超导体K_3C_(60)最近研制成功

据悉,继碳60的合成成功,7月9日,北京大学研究小组又与中科院物理研究所合作,研制成功K_3C_(60),超导起始温度为17.9K,K_3C_(60)是一种碳60的碱金属化合物,一种新型的高温超导体,它的超导转变温度远高于已发现的各种有机超导体。这     

YBa2Cu4O8/La2/3Ca1/3MnO3/YBa2Cu4O8异质结中的超导转变温度

采用对靶溅射技术制备了YBa2Cu4O8/La2/3Ca1/3MnO3/YBa2Cu4O8（Y-124/LCMO/Y-124）异质结, 研究了超导转变温度（TC）随LCMO层厚度（dL）的振荡行为. 当dL＞dLCR时, TC-dL曲线表现出清晰的非单调行为, 而金属-绝缘体转变温度（TMI）仅当dL＞dLCR时才能观测到. Y-124/LCMO/Y-124系统中所存在的这种对中间层的依赖关系, 显示了铁磁和超导耦合间强烈的相互作用.     

氧化铝对Fe－Cu－Zn－K－Al低碳醇合成催化剂性能的影响

 采用N2吸咐，TPR和XRD等表征手段对高温熔融法制备的Fe－Cu－Zn－K－Al催化剂中氧化铝的作用进行了研究．结果表明，当比表面积低于4．0m2／g时，催化剂性能受比表面积的影响非常明显．少量的Al2O3即可有效地增加催化剂的比表面积，提高醇的收率和C2＋OH的选择性；大量的Al2O3虽然能使催化剂的比表面积有所增加，但醇的收率和C2＋OH选择性却显著降低．这是Fe－Cu－Zn－K－Al催化剂中Al2O3同时具有物理作用和化学作用所致．物理作用能有效地增加还原后催化剂的比表面积，提高金属利用率，分散催化剂的活性组分，使其更容易还原，进而提高催化剂活性和选择性．化学作用影响到催化剂的电子性质，从而导致催化剂的活性和选择性降低．TPR和XRD结果表明，在Fe－Cu－Zn－K－Al催化剂中，助剂Al2O3的作用随着其含量的变化而有所不同．当Al2O3含量较低时，其物理作用是主要的；随着Al2O3含量的增加，其化学作用更为明显，甚至导致新物相AlFeO3生成，进而影响催化剂的催化性能．     

C60微电极伏安法研究

自从1990年用电弧法成功地制备出宏观量的C60和C70以来，富勒烯的电化学研究有了迅速的发展．理论研究指出，在一个C60簇化合物中，有六个吡喃环烯单元，可分别得到一个电子使五元环芳香化，从而形成C（n＝1～6）阴离子．Haufler首先报导了C60可逆的两步单电子还原，之后一些作者陆续得到了三步、四步和五步单电子电还原过程．直到达1992年，在使用混合溶剂并控制低温-10℃至5℃和-88℃至60℃条件下，才得到了C60的六步电还原伏安图．富勒烯的微电极伏安法的研究极少见报导．杨汉西等用铂微电极得到了C60三步电还原的稳态伏安图．本文在…     

Molecular mechanics on bonding and non-bonding interactions in (atom@C60)

The interactions between the embedded atom X (X = Li, Na, K, Rb, Cs; F, Cl, Br, I) andC60 cage in the endohedral-form complexes (X@C₆₀) are calculated and discussed according to molecular mechanics from the point of view of the bonding and non-bonding. It is found from the computational results that for atoms with radii larger than Li’s, their locations with the minimum interaction in (X@C₆₀) are at the cage center, while atom Li has an off-center location with the minimum interaction deviation of ~0.05 nm, and the cage-environment in C₆₀ can be regarded as syhero-symmetry in the region with radiusr of ~0.2 nm. It is shown that the interaction between X and C₆₀ cage is of non-bonding characteristic, and this non-bonding interaction is not purely electrostatic. The repulsion and dispersion in non-bonding interactions should not be neglected, which make important contribution to the location with minimum interaction of X, at center or off center. Some rules about the variations of interactions with atomic radii have been obtained. Project supportt:d by the National Natural Science Foundation of China.     

C60离子束撞击固体表面的坍塌沉积(I)共焦显微拉曼光谱研究

Raman spectroscopy was applied to characterize the species deposited from the mass-selected C60 ion beam which was accelerated to 900 eV. The substrates for the deposition were (0001) surface of highly oriented pyrolitic graphite and (111) surface of gold crystal. The species do not exhibit the Raman scattering features of buckminsterfullerene, but displays peaks at 1585 and 1332 cm-1 instead. The former peak is the chararteristic Ranan peak of hexagonal graphite, and the latter can be attributed to the amorphous carbon in sp3 hybridization. The result reveals that C60 was collapsed to form a new phase when it collides on the solid surface.     

Preparation and Characterization of Thin-Film Solar Cells with Ag/C60/MAPbI3/CZTSe/Mo/FTO Multilayered Structures

New solar cells with Ag/C₆₀/MAPbI₃/Cu₂ZnSnSe₄ (CZTSe)/Mo/FTO multilayered structures on glass substrates have been prepared and investigated in this study. The electron-transport layer, active photovoltaic layer, and hole-transport layer were made of C₆₀, CH₃NH₃PbI₃ (MAPbI₃) perovskite, and CZTSe, respectively. The CZTSe hole-transport layers were deposited by magnetic sputtering, with the various thermal annealing temperatures at 300 °C, 400 °C, and 500 °C, and the film thickness was also varied at 50~300 nm The active photovoltaic MAPbI₃ films were prepared using a two-step spin-coating method on the CZTSe hole-transport layers. It has been revealed that the crystalline structure and domain size of the MAPbI₃ perovskite films could be substantially improved. Finally, n-type C₆₀ was vacuum-evaporated to be the electronic transport layer. The 50 nm C₆₀ thin film, in conjunction with 100 nm Ag electrode layer, provided adequate electron current transport in the multilayered structures. The solar cell current density–voltage characteristics were evaluated and compared with the thin-film microstructures. The photo-electronic power-conversion efficiency could be improved to 14.2% when the annealing temperature was 500 °C and the film thickness was 200 nm. The thin-film solar cell characteristics of open-circuit voltage, short-circuit current density, fill factor, series-resistance, and Pmax were found to be 1.07 V, 19.69 mA/cm², 67.39%, 18.5 Ω and 1.42 mW, respectively.     

Annealing Temperature Dependence of the Size of C60 Clusters in C60-Doped Silicon Oxide Films

C₆₀-doped silicon oxide thin films were prepared by spin-coating a viscous solution formed upon soaking at 40°C an acidic toluene/ethanol solution of C₆₀, phenyltriethoxysilane, and tetraethoxysilane with a C₆₀–to–Si molar ratio of 2.5 × 10^–3. The films were submitted to annealing at 300–500°C in Ar to investigate variation in the size of C₆₀ clusters embedded in the films by photoluminescence spectroscopy. The film before annealing was found to contain the clusters consisting of ca. 60 C₆₀ molecules, suggesting that C₆₀ is present well-dispersed in the film. The molecules in the film aggregated to increase the size with increasing annealing temperature, indicating that the molecules diffuse easily in the film upon heating and therefore the size of the clusters is controllable with the annealing temperature.     

He+C60↔(He@C60)的反应势垒研究

The reaction barriers of (He+C60(He＠60)) have been calculated by the quantum-chemical method EHMO/ASED in the following four paths: (1) penetrate through the pentagon on the C60 cage; (2) penetrate through the hexagon on the C60 cage,(3) penetrate through the short bond; (4) penetrate through the long bond. Corresponding to each path, there are two choices: (a) while He penetrate C60 cage, the distances of the C’s which are the most adjacent to He are changed with a planar extension and a concerned window is formed; (b) while He penetrate C60 cage, the distances of the C’s which are the most adjacent to He are changed with a spherical extension and a concerned window is formed. The results are given in Figs. 1-2 and Tables 1-2. It is shown that the reaction through path(4) with choice (a) has the least reaction barrier, being optimum. At that case, a window of 9-membered ring is formed. Because the window extension of C6H6 is more free than that of C60, the barrier of He penetrating through C6H6 will be lower than that of He penetrating through C60.     

Thermal Stability of C60-Methylnaphthalenes Solvates

The crystalline solvates containing fullerenes and (di)methylnaphthalenes were investigated by thermal analyses and X-ray diffraction methods. It was found that C₆₀ with (di)methylnaphthalenes forms two types of stable solvates: either at the molar ratio 1:2 decomposing at temperatures close to 100°C or at 1:1 molar ratio decomposing in the temperature range 120–214°C. Crystalline lattice and thermal stability of the solvates depends on the structure of the solvent molecules. The strong solute-solvent interaction is also manifested by the modification of the C₆₀ absorption spectra in solution. The results are discussed using semiempirical quantum chemistry methods. This revised version was published online in August 2006 with corrections to the Cover Date.     

Thermochemistry of C60 and C70 fullerene solvates

In an effort to improve understanding of dissolution behaviour of fullerenes and their simple chemical derivatives the binary systems of C₆₀, C₇₀ and the piperazine monoadduct of [60] fullerene C₆₀ N₂C₄H₈ with a series of aromatic solvents have been studied by means of DSC. In certain systems solid solvates have been found to be the thermodynamically stable phases relative to saturated solution at room temperature. Identified solid solvates were characterized by their compositions, temperatures and enthalpies of incongruent melting transitions. The regularities in thermodynamic stability of the solvated crystals have been discussed along with dissolution properties of fullerenes and the derivative. Certain correlations have been observed.     

Sol-Gel Synthesis of Metal Nanoclusters-Silica Composite Films

In a program on the development of metal nanoclusters in sol-gel derived thin films, attempts were made to synthesize pure and mixed metal clusters, control the cluster size and increase the volume fract f the clusters. Thus, Ag, Cu and Ag-Cu nanoclusters were prepared in silica films using dip- and spin-coating techniques. The annealing of Ag/SiO₂ films in different atmospheres (air, argon and 5% H₂-95% N₂ gas) caused modifications of Ag nanoclusters resulting in changes in their surface plasmon resonance (SPR) peak positions. The Cu and Ag-Cu codoped films were annealed in reducing atmosphere (5% H₂-95% N₂ gas). In order to prepare Cu nanoclusters of different sizes, the concentrations of Cu in Cu/SiO₂ composite films were varied from 8 to 30 mol% and annealed at 800°C for different times for growth. The size of the Cu nanoclusters was measured from the half band width of Cu SPR peak (appearing within 570–557 nm range) and X-ray diffraction. In this way Cu-nanoclusters of size ranges from about 3.5 to 10 nm (average diameters) were prepared . The Ag-Cu nanocluster-containing silica films show the existence of both Ag and Cu SPR peaks with some blue shifting in comparison with to their pure analogues depending on the Ag:Cu ratio.     

Stabilization of Film Morphology in Polymer‐Fullerene Heterojunction Solar Cells

Abstract

The fixation of film morphology is essential for the long‐term stability of heterojunction polymer photovoltaic (PV) cells. An epoxy‐functionalized fullerene C₆₀ derivative was synthesized for this purpose. This material can be polymerized at acidic conditions and was found to stabilize the phase‐separated morphologies within blended polythiophene–fullerene heterojunction films. The phase stability of the films was characterized by UV‐VIS spectroscopy and optical microscope. Crosslinkable polythiophene derivatives were also prepared but these materials were much less effective in stabilizing film morphology when mixed into PCBM (C61‐butyric acid methyl ester). Heterojunction polymer PV cells were prepared from these materials and their performance was compared with cells made from conventional materials.