纳米结构电学性质的静电力显微镜研究方法

纳米尺度的材料具有许多不同于宏观体材料的奇特的物理和化学特性.了解纳米结构的物性随材料尺寸及形状的变化关系,对于设计和合成具有特定功能的纳米材料有重要的指导意义.静电力显微镜技术为研究微纳米尺度下材料的电学特性提供了强有力的工具.文章介绍了这种测量技术的基本原理,并列举了几种在静电力显微镜基础上发展起来的纳米材料电学性...     

新型高效太阳能电池研究进展

第三代太阳能电池以超高效率、薄膜化、低成本为主要目标,目前发展起来的有多结叠层太阳能电池、中间带太阳能电池、多激子产生太阳能电池、热载流子太阳能电池和热光伏太阳能电池等.文章简要介绍了以上几种新型太阳能电池的工作原理和最新进展,并对其发展前景作了分析和预测.     

Risk models for the Prize Collecting Steiner Tree problems with interval data

Given a connected graph G=(V,E)with a nonnegative cost on each edge in E,a nonnegative prize at each vertex in V,and a target set V′V,the Prize Collecting Steiner Tree(PCST)problem is to find a tree T in G interconnecting all vertices of V′such that the total cost on edges in T minus the total prize at vertices in T is minimized.The PCST problem appears frequently in practice of operations research.While the problem is NP-hard in general,it is polynomial-time solvable when graphs G are restricted to series-parallel graphs.In this paper,we study the PCST problem with interval costs and prizes,where edge e could be included in T by paying cost xe∈[c e,c+e]while taking risk(c+e xe)/(c+e c e)of malfunction at e,and vertex v could be asked for giving a prize yv∈[p v,p+v]for its inclusion in T while taking risk(yv p v)/(p+v p v)of refusal by v.We establish two risk models for the PCST problem with interval data.Under given budget upper bound on constructing tree T,one model aims at minimizing the maximum risk over edges and vertices in T and the other aims at minimizing the sum of risks over edges and vertices in T.We propose strongly polynomial-time algorithms solving these problems on series-parallel graphs to optimality.Our study shows that the risk models proposed have advantages over the existing robust optimization model,which often yields NP-hard problems even if the original optimization problems are polynomial-time solvable.     

Data Collection on and Refinement of Twinned, Non-merohedrally-twinned Methyl 2-Aminopyrazine-3-carboxylate:RLATT for Indexing, and TwinRotMat for De-twinning

The procedure for collecting diffraction data at –173 °C on a twinned specimen of methyl 2-aminopyrazine-3-carboxylate by using the APEX-II software followed by de-twinning the non-merohedrally-twinned reflection data with PLATON is described. De-twinning significantly lowers the R index from 0.141 to 0.038 owing to 49% twinning. Crystal data： C6H7N3O2,monoclinic,P21/c （a = 6.3149（1）,b = 16.5274（2）,c = 6.4544（1） A,β = 95.759（1）°,V = 670.24（2） A^3）.     

B+注入HgCdTe外延材料的红外透射光谱分析

运用多层模型和膜系传递矩阵以及非线性二乘法，模拟了B+注入碲镉汞外延材料的红外透射光谱，结果表明B+注入碲镉汞外延材料的红外透射光谱能够很好地理论再现，并由此获得了结区的自由载流子浓度分布、迁移率、面自由载流子浓度以及折射率和消光系数等相关参量，所得结果与微分Hall法测试的结果是一致的.计算结果也表明B+注入HgCdTe导致红外透射率变化的根本原因是注入层的高载流子浓度的等离子效应改变了该层的折射率和消光系数.     

Carrier Transport Behaviour of Molecular Doped Poly（N—Vinylcabozole）in Polymer Light—Emitting Diodes

Single-layer polymer light-emitting diodes are prepared from blends of poly(N-vinylcarbozole)(PVK) doped with tris(8-hydroxy-quinoline)aluminium(Alq3) of 2wt%(sample a)and 0.2wt%(sample b).The onset of PVK transient electroluminescence(EL) is delayed with respect to that of Alq3 in sample a under pulsed excitation,while the EL onsets of Alq3 and PVK in sample b are simultaneous.The total carrier mobility of the Alq3-rich regions in sample a is larger than that of the PVK-rich regions.However,the total carrier mobility is homogeneous in sample b.the phase image of atomic force microscopy and photoluminescence spectra of samples a and b indicate that the separated phase of samples a and b exists in the PVK-rich and Alq3-rich regions.The variance of the doping concentration and separated phase in blends results in the different carrier transport mobility of Alq3-rich and PVK-rich regions.     

名义组份Bi6Se9Ge4CuOx块材和粉末压实样品的热电势和电导率

采用熔化淬火工艺制备Bi6Se9Ge4CuOx。块材和粉末压实样品均在300℃进行了热处理，该温度远低于玻璃转变温度419℃（由DTA热重分析得知）。无论是末经处理还是热处理后的样品，都具有多相结构。热电势测量结果表明，可能有电子和空穴的导电。载流子的导电类型主要取决于热处理条件。热电势以扩散分量为主，声子曳引可以忽略。跳跃导电是常见的，而半金属行为只在特殊的热处理条件下出现。     

氧含量对Fe掺杂YBCO体系中载流子局域化与离子团簇效应的影响

对YBa₂Cu_3-xFe_xO_y（x=00，01，02 ）和YBa₂Cu_2.8Fe_0.2O_y（y=705—653 ）系列样品的氧含量、霍尔系数和超导电性进 行了系统的研究.结果表明，氧含量的变化对样品中载流子的输运和转移及超导电性有重要 影响；适当增加氧含量可以减缓Cu(1)位元素替代对超导转变温度T_c的抑制；在 CuO₂面上参与输运的载流子（空穴）浓度是影响样品超导电性的关键因素.从电 荷转移模型出发 ，结合掺杂离子引起的载流子局域化和离子团簇效应，对载流子浓度随掺杂量和氧含量的变 化从微观结构方面进行了讨论.元素替代量的增加或者氧含量的降低（相同替代量的情况下 ）都将导致Cu-O链区的有效氧空位增多，导致替代元素的离子团簇效应和载流子局域化效应 趋于增强，这是引起参与输运的载流子浓度下降，进而导致T_c降低的主要原因. 关键词： 氧含量 霍尔系数 载流子局域化 离子团簇效应     

电子型超导体Pr1.85Ce0.15CuO4-δ中Cu位V替代对超导电性的影响

本文研究了Pr1.85Ce0.15CuO4-δ(PCCO)中V4 离子替代Cu2 离子后对其超导电性的影响.Pr1.85Ce0.15Cu1-xVxO4-δ(x=0～0.10)电阻率测量结果显示:微量(x≤0.04)V4 离子替代Cu2 离子可以改善样品的超导电性;随着替代量的增加,体系的超导电性逐渐被抑制,x=0.08时超导电性消失.我们主要从样品的微观结构和载流子浓度两个方面的变化分析了V4 替代Cu2 对PCCO超导电性的影响机制.霍尔系数实验结果表明,替代量较少时,体系中载流子浓度随着x的增加而增加,有助于超导电性的改善,但是当替代量增加到一定程度时,晶格畸变程度的增大和顶点氧的出现,抑制了超导电性.