Pb~(2+)掺杂导致的CaF_2中Yb~(3+)离子三聚体合作发光猝灭

利用978 nm近红外光激发样品Ca F2∶Pb2+,Yb3+,在室温下观察到二价Pb2+离子在383 nm附近的紫外上转换发光。该发射峰对应于Pb2+离子的3P0"1A1g(1S0)跃迁。瞬态光谱测量结果表明:在这个材料体系中,Pb2+离子的激发来自于Yb3+离子三聚体的合作敏化。但是随着Pb2+离子掺杂浓度的提高,Yb3+离子三聚体遭到结构性破坏,导致其合作发光减弱。本文首次利用Pb2+离子掺杂造成Yb3+离子三聚体的结构性破坏,从而引起合作荧光猝灭,并对在Ca F2基质中因其他二价离子的掺入而造成的Yb3+三聚体合作发光猝灭给予了合理的解释。     

一种新型羟基铅配合物的合成及其荧光性质

以3,5-吡唑二甲酸(H₃pdc)为配体,Pb(NO₃)₂为金属盐,在水热反应条件下通过调节pH,合成了一种新的二维羟基Pb配合物--［Pb₂OH(pdc)(H₂O)·H₂O］_n(1),其结构经IR,元素分析和X-射线衍射表征。1(CCDC: 1 469 184)属单斜晶系,P2₁/n空间群,晶胞参数a=10.502(2) , b=9.176 5(2) , c=10.602(2) , β=97.417(7)°, V=1 013.2(3) ³, Z=4, R₁=0.022 4, wR₂=0.045 8, S=1.02。每个不对称结构单元中具有两种不同配位环境的Pb,在同一结构单元中,2个Pb通过羟基O相连,相邻不对称结构单元通过配体连接Pb(Ⅱ)形成二维网络结构。荧光发射光谱研究结果表明：在最大激发波长(264 nm)激发下,1在380 nm, 419 nm和440 nm附近显示出较强的荧光性能。     

烧结温度和升温速率对Pb(Sb1/3Mn2/3)0.05Zr0.47Ti0.48O3压电陶瓷性能的影响

采用传统固相法制备了Pb(Sb1/3 Mn2/3)0.05Zr0.47Ti0.48 O3 (PMS-PZT)压电陶瓷.利用XRD、SEM和EDS等研究PMS-PZT陶瓷体系在烧结过程中形成的过渡液相和形成过渡液相温度(1100℃)附近的升温速率对陶瓷结构、压电和介电性能的影响.结果表明:不同烧结温度下,所有样品均为单一的钙钛矿四方相,过渡液相不会对相的结构有影响,但是当烧结温度较低时,过渡液相在烧结后期以玻璃相在晶界附近富集,对陶瓷的压电和介电性能有很大影响.随着烧结温度和升温速率的升高,PMS-PZT晶粒尺寸增大,晶粒均匀性和规则性得以改善,晶化质量得到提高;d33测试和阻抗分析测试结果表明PMS-PZT样品在1100℃附近以7 ℃·min-1升温速率并在1250℃烧结时具有最好的压电和介电性能:d33 =313 C/N,kp=0.59,Qm=1481,εr=1437,tanδ=0.53;.     

利用EQCM研究铅电极在硫酸和硫酸钠溶液中的反应机理

使用电化学线性扫描伏安(LSV)、循环伏安(CV)和电化学石英晶体微天平(EQCM)方法研究了硫酸和硫酸钠溶液中铅电极表面的反应过程. 伏安曲线和电极表面质量变化结果分析表明,从-1.0 V到-0.4 V正向扫描时,铅在硫酸溶液中生成两种氧化产物,在-0.87 V时生成硫酸铅,在-0.73 V时生成PbO·PbSO₄,然后PbO·PbSO₄转化成硫酸铅,而铅在硫酸钠中的氧化产物只有硫酸铅. 因此,酸性溶液是PbO·PbSO₄形成的必要条件,这进一步揭示了铅酸电池的负极放电机理,也为铅酸电池负极反应过程提供了新的研究方法.     

基于Tessier-AAS法的华中大农区污染红土Pb赋存形态非生物转化机制研究

土壤重金属污染已成为人类面临的共同挑战,典型的重金属污染场地包括金属矿山、公路沿线、工业集中区、农业耕地等。对于事关农业安全生产的大农区,土壤超量重金属往往导致农产品品质下降甚至使用价值丧失,由此造成的经济损失不可估量。实际上,农作物体内累积重金属量与土壤“活性”重金属关系更加密切,这部分重金属主要以可交换态存在,在一定条件下能够与碳酸盐结合态、Fe-Mn氧化态、有机结合态和残渣态相互转换。因此,明确土壤条件对重金属有效性的作用规律,有望从源头上降低重金属对农作物的污染风险。基于前期研究成果,以华中大农区酸性网纹红土为检测对象,采用Tessier连续提取-原子吸收光谱法(AAS)揭示不同条件对红土Pb形态转化的非生物调控机制。结果表明：红土样品Pb总量为32.56 mg·kg-1,低于《土壤环境质量标准》一级标准推荐值,但比全国土壤Pb平均含量要高。不同形态Pb含量分布为残渣态>Fe-Mn氧化态>有机结合态>碳酸盐结合态>可交换态,其中残渣态Pb占Pb总量的54.55%。红土pH值通过改变无机胶体和有机质表面电荷量来控制Pb的结合行为和可交换态含量;不同含水率导致红土氧化还原电位差异,进而影响Pb的形态转化行为。此外,秸秆加入量和老化时间也能改变Pb的形态分布,但残渣态Pb含量始终最高。红土Pb的Muller指数I_geo为0.302 5,表明土样采集区人为污染值得注意。Tessier连续提取-AAS法能有效表征红土Pb赋存形态的非生物转化机制。     

Single‐gap Microelectrode Functionalized with Single‐walled Carbon Nanotubes and Pbzyme for the Determination of Pb2+

Lead is a highly toxic metal, which can persist in the natural environment and enrich in biological bodies. It can cause many severe diseases in the human body even at extremely low concentration. Here, we developed a new biosensor using single‐walled carbon nanotubes (SWNTs) modified with a specific Pbzyme (Pbzyme/SWNTs/FET) to detect lead ion (Pb²⁺), which can monitor the lead pollution. This biosensor used 3‐aminopropyltriethoxysilane to immobilize SWNTs on the area between the source and the drain of single‐gap microelectrode (FET), and the duplex DNA (Pbzyme) consisted of DNAzyme (GR‐5) and complementary DNA (CS‐DNA) was functionalized with the SWNTs’ surface through a peptide bond. The use of GR‐5 DANzyme and Pb²⁺ to form a stable complex structure to cleave the CS‐DNA can change radically the Pbzyme's structure on the SWNTs’ surface, which will further affect the number of carriers in SNWTs and the conductivity of the Pbzyme/SWNTs/FET. The change in conductivity can be used to evaluate the Pb²⁺ concentration. Under the optimal conditions, the relative resistances presented a positive correlation with the Pb²⁺ concentrations, showing a good linear relationship in the range of 10 pM to 50 nM, where the linear regression equation was y=10.104log [C_Pb]+5.8656, and the detection limit was 7.4 pM. Finally, the biosensor was applied to measure the Pb²⁺ contents in the soil collected from the forest grass green belt and paint, and the results were compared with the results of atomic fluorescence spectrometry.     

电感耦合等离子体原子发射光谱法(ICP-AES)测定铜砷滤饼中的Pb、Fe、Bi三种元素

采用硝酸、盐酸、氢氟酸、高氯酸分解样品,氢溴酸-盐酸挥发消除砷基体,优化仪器测定参数,选取最佳工作条件,建立了电感耦合等离子体原子发射光谱(ICP-AES)法测定铜砷滤饼中Pb、Fe、Bi元素的分析方法。其测定范围为：ω(Pb):0.12%~2.09%;ω(Fe):0.081%~2.10%;ω(Bi):1.20%~6.14%。各元素检出限为Pb:0.010μg/mL;Bi:0.006μg/mL;Fe:0.003μg/mL。加标回收率为95.5%~101.7%。该方法简便,准确,可靠,适用于铜砷滤饼中Pb、Fe、Bi元素的同时测定。     

微波消解ICP-AES法测定ABS中Pb、Cd、Hg

以ABS塑料为研究对象,采用微波消解法进行样品的前处理,使用电感耦合等离子体发射光谱法测定ABS塑料中Pb、Cd、Hg,结果表明,Pb、Cd、Hg加标回收率均在95~105%之间,测试精密度均小于3%,该方法在缩短样品前处理时间的同时得到较高的元素消解回收率和较为理想的精确度,适用于ABS塑料中重金属含量的快速测定。     

Spectral and kinetic characteristics of CdI<Subscript>2</Subscript> and CdI<Subscript>2</Subscript>:Pb scintillators

We have studied the effect of lead dopant on the optical absorption, photoluminescence, and x-ray luminescence spectra, and the scintillation characteristics of CdI₂ at room temperature. The crystals for the study were grown by the Stockbarger-Bridgman method. Activation of CdI₂ from the melt by the compound PbI₂ leads to the appearance in the absorption spectra in the near-edge region of an activator band at 395–405 nm, which is interpreted as an A band connected with electronic transitions from the ¹S₀ state to the ³P₁ levels in the Pb²⁺ ion. For x-ray excitation, CdI₂:Pb²⁺ crystals with optimal dopant concentration (∼1.0 mol%) are characterized by a light yield with maximum in the 570–580 nm region that is an order of magnitude higher than for CdI₂ crystals in the 490–500 nm band. For α excitation, the radioluminescence kinetics for cadmium iodide is characterized by a very short (∼0.3 nsec) rise time and fast decay of luminescence, with τ₁ ≈ 4 nsec and τ₂ = 10–76 nsec. Depending on the conditions under which the crystals were obtained, the fast component fraction is 95%–99%. The crystal is characterized by a similar scintillation pulse in the case of excitation by x-ray pulses. The radioluminescence pulse shape for CdI₂:Pb in the decay stage is predominantly exponential, with luminescence decay time constants τ₁ ≈ 10 nsec and τ₂ = 200–250 nsec. This system is characterized by low afterglow, at the level for the Bi₄G₃O₁₂ scintillator. We have demonstrated the feasibility of using CdI₂:Pb as a scintillator for detecting α particles. Translated from Zhurnal Prikladnoi Spektroskopii, Vol. 75, No. 6, pp. 825–830, November–December, 2008.     

Application of interference microscopy to the study of hologram build-up in LiNbO3 crystals

Interference microscopy was applied to direct microscopic observation of temporal evolution of phase holograms in LiNbO₃:Fe photorefractive crystals. First a hologram was recorded in the sample, and diffraction efficiency was monitored during hologram build-up using inactinic laser light. Thus kinetics of hologram build-up could be determined. The initial hologram was erased using white light. Then a series of write-erase cycles were performed with increasing exposure times. Holograms were observed by interference microscope after each exposure. The time elapsed between the exposure and the microscopic observation was negligible compared to the relaxation time of the hologram. The obtained temporal evolution of the grating profile gives a deeper insight into the physical mechanism of hologram formation in photorefractive materials than simple diffraction efficiency measurements. A congruently grown sample of LiNbO₃ doped with 10⁻³ mol/mol Fe in melting was studied by this method. Sample thickness was set to 300 μm to allow correct microscopic observation. Plane-wave holograms were recorded in the samples using an Ar-ion laser at λ = 488.0 nm of grating constants of 3, 6.5 and 8.8 μm.