Degradation of reactive,acid and basic textile dyes in the presence of ultrasound and rare earths [Lanthanum and Praseodymium]

Degradation of five textile dyes, namely Reactive Red 141 (RR 141), Reactive Blue 21 (RB 21), Acid Red 114 (AR 114), Acid Blue 113 (AB 113) and Basic Violet 16 (BV 16) in aqueous solution has been carried out with ultrasound (US) and in combination with rare earth ions (La³⁺ and Pr³⁺). Kinetic analysis of the data showed a pseudo-first order degradation reaction for all the dyes. The rate constant (k), half life (t_1/2) and the process efficiency (φ) for various processes in degradation of dyes under different experimental conditions have been calculated. The influence of concentrations of dyes (16–40 mg/L), pH (5, 7 and 9) and rare earth ion concentration (4, 12 and 20 mg/L) on the degradation of dyes have also been studied. The degradation percentage increased with increasing rare earth amount and decreased with increasing concentration of dyes. Both horn and bath type sonicators were used at 20 kHz and 250 W for degradation. The sonochemical degradation rate of dyes in the presence of rare earths was related to the type of chromophoric groups in the dye molecule. Degradation sequence of dyes was further examined through LCMS and Raman spectroscopic techniques, which confirmed the sonochemical degradation of dyes to non-toxic end products.     

Raman spectrum study of graphite irradiated by swift heavy ions

Highly oriented pyrolytic graphites are irradiated with 40.5-Me V and 67.7-Me V ^112Sn-ions in a wide range of fluences： 1×10^11 ions/cm^2–1×10^14ions/cm^2. Raman spectra in the region between 1200 cm^-1 and 3500cm^-1 show that the disorder induced by Sn-ions increases with ion fluence increasing. However, for the same fluence, the amount of disorder is greater for 40.5-Me V Sn-ions than that observed for 67.7-Me V Sn-ions, even though the latter has a slightly higher value for electronic energy loss. This is explained by the ion velocity effect. Importantly, ～ 3-cm^-1frequency shift toward lower wavenumber for the D band and ～ 6-cm^-1 shift toward lower wavenumber for the 2D band are observed at a fluence of 1×10^14 ions/cm^2, which is consistent with the scenario of radiation-induced strain. The strain formation is interpreted in the context of inelastic thermal spike model, and the change of the 2D band shape at high ion fluence is explained by the accumulation of stacking faults of the graphene layers activated by radiation-induced strain around ion tracks. Moreover,the hexagonal structure around the ion tracks is observed by scanning tunneling microscopy, which confirms that the strains near the ion tracks locally cause electronic decoupling of neighboring graphene layers.     

原位微区同步辐射X射线荧光和近边吸收谱研究拟南芥幼苗及根际土壤中铅分布与形态特征

为了从组织和器官水平研究植物在铅锌矿山开采区尾矿坝土壤中植物中毒和胁迫机制,使用同步辐射微束X射线荧光技术(μ-SRXRF)研究了K,Ca,Mn,Fe,Cu,Zn,Pb等元素在云南某铅锌矿区尾矿坝土壤中生长的拟南芥幼苗中的分布特征。发现Pb易富集于植物根部,也容易富集在植物顶端叶芽部位,这是很多研究没有发现的。整株幼苗中Pb都与Mn形成明显的竞争分布特征。导致植株中毒凋亡的原因可能是Pb造成的拟南芥顶端幼芽的氧化压力,以及Pb分布对Mn等植物必需元素的吸收和分布的抑制。为研究Pb在土壤中的形态和植物可利用性,针对拟南芥及其根际土壤中开展了Pb L3边X射线吸收近边精细结构谱(XANES)研究,发现尾矿坝土壤种植的拟南芥根际土壤Pb主要以PbO(64.2%),Pb(OH)2(28.8%),Pb3O4(6.3%)形式存在,而非Pb矿物矿石或有机Pb形式存在,本尾矿坝土壤中Pb的植物可利用水平不高。进一步开展土壤中Pb进入植物的过程以及该过程中Pb的形态发生的变化,尤其是溶解性有机质在其中的角色,是开展重金属胁迫下植物中毒和解毒机制研究的重要前提。     

立方相Na_(1/2)Bi_(1/2)TiO_3和K_(1/2)Bi_(1/2)TiO_3的电子结构和结构不稳定性的第一性原理比较研究

采用基于密度泛函理论的第一性原理方法比较研究了Na1/2Bi1/2TiO3和K1/2Bi1/2TiO3的电子结构、离子位移势能面和Γ声子等性质.结果表明,Na1/2Bi1/2TiO3和K1/2Bi1/2TiO3的电子结构很相似,价带由O 2p电子态主导并包含部分Ti 3d和Bi 6p电子态,导带低能部分由Ti 3d空轨道构成;K取代Na后其Ti—O和Bi—O键的键强略有增加.两者的离子位移势能面也很接近,O离子的偏心位移对结构不稳定性起主导作用,且K取代Na后其作用增强.Γ声子都存在3个软模,分析表明软模主要来自O6基团的振动,K取代Na后A2u软模发生硬化.     

ZnS：Mn/SiO2量子点的表面聚乙烯吡咯烷酮修饰及其应用于海水中铅离子检测

制备了二氧化硅壳层修饰的ZnS：Mn量子点,基于聚乙烯吡咯烷酮（PVP）与二氧化硅表面硅羟基的作用,在纳米复合微粒表面进行了PVP的修饰,得到了在海水中荧光性能及胶体稳定性良好的ZnS：Mn/SiO₂/PVP 量子点。在Pb²⁺对所制备纳米微粒具有荧光猝灭效应的基础上,建立了用ZnS：Mn/SiO₂/PVP 量子点作为荧光探针检测海水中微量铅离子的新方法。研究表明,量子点浓度为10^-3 mol/L时,海水中离子浓度在10~100 μmol/L范围内与ZnS：Mn/SiO₂/PVP量子点荧光猝灭强度呈良好的线性关系,相关系数为0.994 6,检出限为8×10^-7 mol/L。     

近红外发射CdSeTe量子点测定铜离子

以CdCl₂·2.5H₂O、Na₂SeO₃、Na₂TeO₃和N₂H₄·H₂O为反应物,以3-巯基丙酸（MPA）为稳定剂制备CdSeTe量子点。与CdTe量子点相比,CdSeTe合金量子点的发射光谱明显红移,发光颜色可扩展至近红外波段范围。基于铜离子能有效猝灭CdSeTe合金量子点荧光的特性,开发了一种用近红外CdSeTe量子点为荧光探针测定铜离子浓度的分析方法。在最佳实验条件下,该方法的线性检测范围为10～200 μg/L,检测上限为1.13 μg/L。应用于实际样品中铜的测定,结果与ICP测定值非常吻合。     

Er3+掺杂Ge-Ga-S-KBr硫卤玻璃的中红外发光和多声子弛豫的研究

用熔融急冷法制备了系列不同Er3+离子掺杂浓度的Ge-Ga-S-KBr硫卤玻璃,测试了样品折射率、吸收光谱、中红外荧光光谱。通过吸收光谱计算了Er3+离子吸收谱线的振子强度,应用Judd-Ofelt理论计算分析了Er3+离子在Ge-Ga-S-KBr硫卤玻璃中的强度参数Ωi ( i = 2 , 4 , 6) 、自发辐射跃迁几率A、荧光分支比?和辐射寿命?rad等光谱参数。研究了808nm激光泵浦下样品中红外荧光特性与掺杂浓度之间变化关系,并用Futchbauer-Ladenburg公式分别计算了2.8?m处的受激发射截面。结果表明,在808nm 激光泵浦下观察到了2.8?m中红外荧光,分别对应于Er3+： 4I11/2?4I13/2跃迁,当Er3+离子掺杂浓度从0.4wt%增加到1.0wt%时,中红外荧光强度都随相应增加,计算的Er3+:4I11/2?4I13/2跃迁多声子驰豫速率分别为37 s-1。     

塑料闪烁光纤阵列成像探测器在高能X射线辐照下的串扰分析

采用蒙特卡罗方法对闪烁光纤阵列探测器在高能X射线入射下的串扰进行了模拟研究,并且分析比较了加铅层对串扰的影响.研究中采用对表征成像系统空间分辨率参量——调制传递函数进行模拟分析和比较,得到在光纤阵列之间加入不同铅层厚度后对系统调制传递函数参量曲线的影响.研究结果表明:在高能射线下,采用闪烁光纤阵列作为成像探测器存在严重的次级粒子相互串扰的现象,而在阵列之间加入铅介质能够减少这种效应;但另一方面,若所加铅层太厚又会导致成像探测器像素过大而使得空间分辨率下降.通过模拟计算得出:只要在阵列之间加入适当厚度的铅介质,既可以有效抑止阵列之间次级粒子的串扰,同时又能提高闪烁光纤阵列探测器系统的空间分辨率.     

团簇增强的纳秒激光电离产生Xez+(z≤20)高价离子

利用功率密度为1011—1012W·cm-2的1064nm纳秒激光电离氙原子团簇，在飞行时间质谱中观察到电离态高达+20的高价离子.不同脉冲束位置实验表明，仅当激光作用于分子束的中段时，才能观察到高价离子，且高价离子的强度随束源压力的增加而迅速增强.实验结果表明束中大尺寸团簇的存在与高价离子的形成密切相关.讨论了高价离子产生的可能机理. 关键词： 氙 纳秒激光 高价离子 飞行时间质谱