紫外吸收光谱研究4,4′-二硝基二苯乙烯-2,2′-二磺酸稀溶液的光致顺反异构

首次发现并证实了在4,4′-二硝基二苯乙烯-2,2′-二磺酸稀溶液中存在顺反异构现象。采用紫外吸收光谱对其稀溶液的光致顺反异构进行了研究。结果表明，溶液的浓度越稀，光照时间越长，反式异构体转化成顺式异构体越快、越多。     

溶胀后的弹性印章进行毛细微模塑

用溶胀后的聚二甲基硅氧烷弹性印章进行毛细微模塑,得到了聚苯乙烯丙酮溶液的微四方点阵图案．较少的PS溶液滴加量会造成孤立不相连的微点阵图形．同时还获得了由于在收缩过程中各部分溶剂挥发速度不一造成的特殊的微点阵图案．     

侧链含查尔酮基团的聚(甲基)丙烯酸酯的光交联特性

采用红外光谱、热重分析、紫外光谱和荧光光谱对侧链含查尔酮基团的聚（4-甲基丙烯酰氧基-4'-二甲氨基查尔酮）（PMADMAC）和聚（4-丙烯酰氧基查尔酮）（PAC）的光交联特性进行了研究。随着光照时间的增加,PMADMAC和PAC聚合物光致环加成反应迅速进行,波长短的紫外线更易使得聚合物发生[2+2]环加成反应。与溶液状态相比,固体薄膜状态下的光交联反应速率较慢。PMADMAC聚合物更容易发生光致环加成反应,其光交联速率要比PAC聚合物快,环加成反应也更彻底。采用荧光光谱研究了聚合物的发光特性,发现PAC聚合物无荧光,而PMADMAC聚合物具有溶剂极性敏感的荧光特性。在PMADMAC聚合物的稀溶液中,随着365 nm紫外光照时间的增加,荧光强度迅速降低,其荧光特征波长在紫外光照射后发生蓝移。 PMADMAC和PAC聚合物的热稳定性较好,光交联后形成热不稳定的环丁烷结构,其热稳定性有所降低。     

用微模塑直接在聚合物曲面上制备微图形

用聚二甲基硅氧烷制备的 ,表面复制有微图形的“弹性印章”直接在聚乙烯 ,聚丙烯 ,聚苯乙烯和聚甲基丙烯酸甲酯等热塑性聚合物表面上进行热微模塑 ,无需复杂设备并可在普通实验室条件下 ,复制微图形 ,甚至在小试管外壁的曲面上或在用毛细管形成的微突起表面上也能制备出微曲面图形 .讨论了不同聚合物对生成微图形的影响 ,认为结晶性聚合物以及在温度变化时有较大收缩率的聚合物在微模塑中难以获得清晰图形 .无定形聚合物如聚苯乙烯和聚甲基丙烯酸甲酯等能够获得清晰的微结构     

9,9-二-(3-丙基酰胺-2-甲基丙磺酸)芴共聚物的合成及荧光发光性能

利用迈克尔加成反应合成了2,7-二溴-9,9-二-(3-丙基酰胺-2-甲基丙磺酸)芴(FSO3H),并通过Suzuki偶合反应制备了9,9-二-(3-丙基酰胺-2-甲基丙磺酸)芴-9,9-二己基芴共聚物(PF6SO3H)和9,9-二-(3-丙基酰胺-2-甲基丙磺酸)芴-4,4'-联苯共聚物(PFDBSO3H)。通过核磁共振氢谱(1H NMR)、凝胶渗透色谱(GPC)、紫外-可见吸收光谱对聚合物的结构进行了表征,利用荧光发射光谱对聚合物在各种条件下的荧光发光性能进行了研究。结果表明,上述两种磺酸型聚芴已被成功合成,这些聚合物具有较高的分子量并能够很好地溶于甲醇和水/醇混合溶剂中。荧光发光光谱研究表明:溶剂的极性、溶液的浓度和p H值、溶液中的金属离子都对磺酸型聚芴的发光性能有很大的影响。荧光发射光谱随着溶剂极性的增加逐渐红移。荧光强度随着溶液浓度的增加先增加后降低。当溶液p H从1增加到7.5时,荧光强度逐渐增加;当p H从7.5增加到12.5时,荧光强度降低直至猝灭。离子猝灭剂Mv+、Ag+、K+、Na+和Li+等对两种聚合物具有明显的猝灭效应,且对PF6SO3H的猝灭效应比对PFDBSO3H更强,这与磺酸型聚芴分子的刚性及离子的相互作用有关。     

聚环氧乙烷在水和叔丁醇溶液中分子构型变化的研究

在聚合物溶液中,聚合物单体和溶剂分子之间的相互作用会影响聚合物高分子的尺寸和结构。本文使用动态光散射实验系统研究了聚环氧乙烷在水+TBA二元混合溶液中的分子尺寸变化,实验结果表明聚环氧乙烷分子会呈现出收缩-膨胀的奇异性构型变化。本文也系统分析了产生该现象的原因,依次分析了在二元混合溶液中可能对聚合物分子尺寸产生影响三个原因:溶剂非理想性影响(Shultz-Flory理论)、临界涨落影响以及水+醇溶液所呈现出来的奇异性性质。结合这三个因素,本文较好地解释了实验所观测到的奇异现象。     

二氧化钛修饰的微结构聚合物光纤预制棒制备及其在光催化中应用的探索研究

首次用二氧化钛(TiO₂)纳米材料修饰的547孔微结构聚合物光纤(MPOF)二次预制棒作为阵列化微管式光催化反应器对亚甲基兰的光催化分解进行研究.将高光催化活性的P25型二氧化钛纳米粒子均匀分散在TiO₂溶胶中,对547孔微结构聚合物光纤孔洞内壁进行铺膜,得到了负载光催化剂的阵列化微管材料.该TiO₂MPOF有序复合的阵列化微管不仅对二氧化钛纳米粒子起到负载作用,还可以作为光波导介质(rolling-up薄膜波导,聚光、导光进入二氧化钛薄膜层)、污染物反应流体通道.以有机染料亚甲基兰为模拟污染物,研究了TiO₂负载量、亚甲基兰的初始浓度及溶液pH值等因素对光降解效果的影响.该反应器547个孔道的内表面用于负载光催化剂,不仅增加了固-液接触面积,也提高了光的吸收效率,从而提高了光催化效率.迄今为止,这种兼具导光、聚光、传质、负载功能于一体的光催化反应器还未见报道.     

制备低密度聚-4-甲基-1-戊烯泡沫中的热性能研究

 在聚-4-甲基-1-戊烯(pmp)低密度泡沫的制备中,利用示差扫描量热（DSC）分析仪对pmp聚合物在均四甲苯/萘所组成的溶剂/非溶剂二元体系中的凝胶化过程进行在线测量。测定了它的凝胶化范围以及凝胶化温度与冷却速率和pmp在溶剂/非溶剂体系中所占比例的关系。利用热重-示差扫描量热（TG-DSC）系统对所制备的低密度pmp泡沫的热性能进行了分析,得到了泡沫密度变化对热稳定性等的影响。     

基于动态溶胀法制备中空聚合物微球

以表面带正电荷的m级聚苯乙烯微球为种子,经过甲苯、二乙烯基苯溶胀,聚合与包覆等过程制备了直径约5 m的中空聚合物微球。研究了溶剂类型、溶剂用量对动态溶胀法制备的中空聚合物微球粒径、分布和结构的影响,讨论了中空聚合物微球的形成机理。结果表明:添加一定量甲苯、二甲苯等挥发性溶剂是动态溶胀法形成中空聚合物微球的前提;甲苯用量越多,溶胀后形成的中空结构越明显,孔径越大;选择低溶解性的二甲苯溶剂更有利于中空结构的形成。     

交联β-环糊精-可溶性淀粉聚合物的微球吸附防晒剂行为

以对甲氧基肉桂酸异辛酯(OMC)和交联β-环糊精-可溶性淀粉聚合物微球为原料,以OMC包封率和载料质量分数为评价指标,通过单因素设计对制备交联β-环糊精-可溶性淀粉聚合物微球吸附OMC的工艺条件进行了优化.结果表明:OMC:交联β-环糊精-可溶性淀粉聚合物微球=1∶100(质量比),50％乙醇溶液为溶剂,25℃下反应60min,包封率为63.63％,载料质量分数6.59％;在0-24h内,OMC在β-环糊精-可溶性淀粉聚合物微球中的累积释料率符合零级释放规律.     

Speckle characteristics of a broad-area VCSEL in the incoherent emission regime

We present a technique to reduce the speckle contrast of a NIR broad-area VCSEL based on the spatially incoherent emission regime that can be obtained when using the proper driving conditions. We evaluate the efficiency of this technique to reduce the speckle contrast by comparing it with the speckle characteristics in multimode emission under cw operation. Depending on the illumination setup, the incoherent emission regime can lead to a strongly reduced speckle contrast down to 1.3%. This is in agreement with estimates of the expected speckle contrast reduction when three contrast reducing effects are taken into account. These low contrast values make the investigated sources attractive for several applications that suffer from speckle noise.     

Structural characterization of ultrathin Cr and Sc films for soft X-ray mirrors

The structure of multilayers of ultrathin scandium (Sc) and chromium (Cr) films has been characterized by means of transmission electron microscopy (TEM). Face centered cubic Sc was found both in magnetron sputtered thin Sc layers on Si(0 0 1) and in Cr/Sc multilayers for soft X-ray mirrors. The single Sc and Cr layers are polycrystalline with randomly oriented grains, while Sc and Cr within the Cr/Sc multilayer show a strong [0 0 1] texture in the deposition direction. From high-resolution images the orientation-relationship at the Cr/Sc interfaces could be deduced as: Sc_[110]//Cr_[100] and Sc_[010]//Cr_[110], which was confirmed by image simulations.     

Optical transmission through an interface between subwavelength slits

This paper studies optical transmission through an interface between two slits with different widths in a sheet composed of an ideal conductor. Such a structure is of potential use in fabricating optical diode and may be the simplest one compared to other designs. Our calculations show that there is a critical wavelength. When the light wavelength is below the critical wavelength, the transmissivity is unidirectional. The expression of the stable transmissivity as a function of the ratio of the widths of the two slits was obtained analytically. Particularly, at the critical wavelength, the transmissivities are zero. This phenomenon has great potential for application in the manufacture of wavelength blockers.     

Effect of Ir(pq)2acac doping on CBP in phosphorescence organic light-emitting diodes

Doping is one of the most powerful methods amongst the various performance improvement ways. Doping affects the energy levels of the host layer by the energy level of the dopant. This allows the energy bandgap to be adjusted to a desired level and thus generates light corresponding to that energy level. Alternatively, it can act as an energy barrier between the interfaces to change the flow of carriers. In this study, the voltage dependences of undoped and doped devices were observed. Bis(2-phenylquinoline) iridium(III) (acetylacetonate) (Ir(pq)₂acac) was doped in 4,4′-N, N′-dicarbazole-biphenyl (CBP) as the emission layer. The light intensity changes with the doping concentration, and the efficiency was also studied. When a high voltage was applied, the effect of triplet-triplet annihilation (TTA) adversely affected the electron-hole recombination. We analyzed the optimal operating conditions and the effect of doping concentration on OLEDs.     

Grain boundary potential and charge density at grain boundaries of chemically prepared thin silver sulfide films

The grain boundary potential and interface state charge density at the grain boundaries of silver sulfide (Ag₂S) thin films prepared by chemical conversion of cadmium sulfide (CdS) films have been determined from the dc resistance of the material and are found to be sensitive to annealing. A reduction in the grain boundary potential and the grain boundary charge density of the film has been noticed when the source CdS film is annealed at different temperatures prior to chemical conversion. The variation in the grain boundary charge density of the grown Ag₂S film with source annealing temperature has been found to be similar to that of thin cadmium sulfide film, reported earlier. An additional low temperature heat treatment of the sample results in an enhancement in the charge density at the grain boundaries. The change in the silver vacancy and/or oxygen and sulfur content of the films as revealed from the energy dispersive spectra of the films suggests possible role of film composition on the grain boundary charge density.     

三螺旋DNA分子Poly(dT)·Poly(dA)·Poly(dT)碱基振动模式

利用晶格动力学方法计算了三螺旋 DNA分子 poly(d T)· poly(d A)· poly(d T)碱基振动模式 ,并根据势能分布矩阵对碱基振动模式进行了指定。计算的模式频率同拉曼光谱实验相符合     

XYZ particles at Belle

In this paper, I review recent progress in the study of the XYZ particles at Belle. I only focus on studies with charmonium and one or more light mesons in the final states. This covers the X(3872), X(3915),Y(4140), X(4350), and the charged Z states.     

Belle实验观测到新类粲偶素结构

利用在Υ(nS)(n=1,2,4,5)共振态及其附近采集的大量数据,Belle实验测量了末态中含两个矢量粒子的双光子过程γγ→J/ψ和ωJ/ψ.在这两个过程中,发现了两个窄共振结构X(4350)和X(3915).这两个新结构的性质目前尚不清楚,可能是普通粲偶素粒子,也可能是含一对粲夸克和一对轻夸克的四夸克态,或含一对粲夸克和一个激发胶子的混杂态,或是由其他未知的动力学原因造成的奇特结构.Belle同时发现在γγ→J/ψ过程中,不存在显著的Y(4140)的信号,实验结果与将Y(4140)解释为四夸克态的部分理论预期有较大差异.     

Effect of swift heavy ion irradiation on photoluminescence properties of ZnO/PMMA nanocomposite films

We report a study on the SHI induced modifications on structural and optical properties of ZnO/PMMA nanocomposite films. The ZnO nanoparticles were synthesized by the chemical route using 2-mercaptoethanol as a capping agent. The structure of ZnO nanoparticles was confirmed by XRD, SEM and TEM. These ZnO nanoparticles were dispersed in the PMMA matrix to form ZnO/PMMA nanocomposite films by the solution cast method. These ZnO/PMMA nanocomposite films were then irradiated by swift heavy ion irradiation (Ni⁸⁺ ion beam, 100 MeV) at a fluence of 1×10¹¹ ions/cm². The nanocomposite films were then characterized by XRD, UV-vis absorption spectroscopy and photoluminescence spectroscopy. As revealed from the absorption spectra, absorption edge is not changed by the irradiation but the optical absorption is increased. Enhanced green luminescence at about 527 nm and a less intense blue emission peak around 460 nm were observed after irradiation with respect to the pristine ZnO/PMMA nanocomposite film.     

The effect of phonon anisotropic scattering on the thermal conductivity of silicon thin films at 300K and 400K

Previous studies have shown that anisotropy in phonon transport exist because of the difference in phonon dispersion relation due to different lattice directions, as observed by a difference in in-plane and cross-plane thermal conductivities. Our current work intends to study the effect of anisotropy scattering on silicon thermal conductivity at 300 K and 400 K. We adopt the Henyey and Greenstein probability density function in our phonon Monte Carlo simulation to investigate the effect of highly forward and backward scattering events. The impact of applying the anisotropy scattering using this approach is discussed in detail. While the forward and backward scattering will increase and decrease thermal conductivity respectively, the extent of the effect is non-linear such that forward scattering has a more obvious effect on thermal conductivity than backward scattering.