杯芳烃修饰玻碳电极直接电位法测定铅离子

杯芳烃是一类苯酚与甲醛缩合而成的新型大环化合物.因为易于合成并可在母体上修饰功能团,使其具有特殊的性质而倍受关注~([1,2]).     

固相萃取-柱后衍生-反相高效液相色谱法测定脱水蒜粉中的亚硫酸盐

建立了测定脱水蒜粉中亚硫酸盐含量的柱后衍生-反相高效液相色谱分析方法.样品用HCl/甘露醇缓冲溶液提取,经固相萃取(SPE)小柱净化本底并富集待测物后,与甲醛缓冲液反应生成稳定的化合物羟甲基磺酸盐,采用高效液相色谱柱及柱后衍生分离,紫外检测器检测,外标法定量.色谱柱为:Agila Venusil MP-C18(4.6 mm×250 mm),流动相为0.005 mol/L四丁基氢氧化铵离子溶液(pH 4),检测波长为450 nm,结果表明,检出限为2.0 mg/kg,在0.1～10.0 μg/mL范围内线性关系良好,相关系数R2=0.9998,样品添加回收率为86.5%～97.6%,RSD为2.2%～4.0%(n=5).     

Experimental Determination of the Landé g-Factors for 5s~2 ~1S and 5s5p ~3P States of the ~(87)Sr Atom

We present an experimental determination on the Lande g-factors for the 5 s~2 ~1 S_0 and 5 s5 p ~3 P_0 states in ultra-cold atomic systems, which is important for evaluating the Zeeman shift of the clock transition in the ~(87)Sr optical lattice clock. The Zeeman shift of the 5 s5 p ~3 P_0-5 s~2 ~1 S_0 forbidden transition is measured with the π-polarized andσ~±-polarized interrogations at different magnetic field strengths. Moreover, in the g-factor measurement with the σ~±-transition spectra, it is unnecessary to calibrate the external magnetic field. By this means, the ground state 5 s~2 ~1 S_0 g-factor for the ~(87)Sr atom is-1.306(52) ×10~(-4), which is the first experimental determination to the best of our knowledge, and the result matches very well with the theoretical estimation. The differential g-factorδg between the 5 s5 p~3 P_0 state and the 5 s~2 ~1 S_0 state of the ~(87)Sr atoms is measured in the experiment as well,which are-7.67(36) ×10~(-5) with π-transition spectra and-7.72(43) X 10-5 with σ~±-transition spectra, in good agreement with the previous report [Phys. Rev. A 76(2007) 022510]. This work can also be used for determining the differential g-factor of the clock states for the optical clocks based on other atoms.     

考虑密度与温度耦合关系的非结构网格SIMPLEC算法

提出一种新的密度压力速度和温度耦合的算法,使用静焓方程构造温度修正量与压力修正量之间的关系,类似Rhie-Chow方法用动量方程插值,网格面上的温度压力修正量插值采用能量方程的形式.CGNS API(CFD General Notation System Application Programming Interface)作为非结构化网格求解器的前处理和后处理,基于网格的FVM(Finite Volume Method)作为偏微分方程求解方法.燃烧模拟采用Arrinius-Eddy Dissipation模型.最后给出两个算例作为说明.     

纳米银六角阵列在掺氧氮化硅中的局域表面等离激元共振特性仿真

通过COMSOL Multiphysics 和 Lumerical FDTD solution对不同尺寸纳米银六角阵列在非晶态掺氧氮化硅(a-SiN_x:O)介质中的局域表面等离激元共振(LSPR)特性进行仿真, 计算结果表明半径为25 nm的纳米银六角阵列形成的局域表面等离激元(LSP)与厚度为70 nm的a-SiN_x:O的蓝光发射(460 nm)的共振效果最为显著, 随着纳米银颗粒尺寸的增大其消光共振峰红移. 在460 nm波长激发下半径为25 nm的纳米银阵列在a-SiN_x:O中的极化强度和表面极化电荷的分布模拟证明了该阵列在460 nm激发下形成的LSP为偶极子极化模式, 通过对该尺寸的纳米银阵列的LSP 在a-SiN_x:O中的最强垂直辐射空间计算, 获得了银颗粒上方a-SiN_x:O的最佳厚度为30 nm, 仿真结果对硅基蓝光发射器件(450–460 nm)的设计提供了重要的理论参考.     

High-temperature sensor using a Fabry-Perot interferometer based on solid-core photonic crystal fiber

A micro Fabry-Perot interferometer(M-FPI) is constructed by splicing a short section of polarizationmaintaining photonic crystal fiber(PM-PCF) to an end-cleaved single-mode fiber with controllable offset. Due to the high effective optical path difference induced by the solid core of the PCF,the M-FPI has an ultrasmall cavity of approximately 110μm.The temperature sensitivity within a range from 33℃to approximately 600℃is measured to be 13.8 pm/℃,which shows good agreement with the theoretical result.This proposed sensor has the advantages of ultracompact size and high stability.Therefore,it is suitable for various space-limited sensing applications in harsh environments.     

锶玻色子的“魔术”波长光晶格装载实验研究

光晶格中性原子光钟的不确定度已达到10^-18量级. 本文介绍了碱土金属锶原子玻色子⁸⁸Sr在“魔术”波长处的一维光晶格装载, 实现冷锶原子的囚禁并使锶原子的钟跃迁能级(5s²) ¹S₀-(5s5p) ³P₀在此波长处的交流斯塔克光频移一致. 实验中半导体激光器产生“魔术”光波长(813 nm), 通过实验搭建光学驻波场并获得晶格激光聚焦光束, 束腰半径为38 μm. 经过一级冷却和二级冷却后温度约为2 μK的冷锶原子被此“魔术”波长光晶格囚禁. 通过实验测量得到锶原子玻色子⁸⁸Sr光晶格寿命为270 ms, 数目约为1.2×10⁵, 温度在3.5 μK左右, 此外研究了晶格光功率对晶格囚禁原子数目及温度的影响作用. 原子的光晶格装载为后续的钟跃迁提供了长的探测时间, 为进一步的光钟闭环提供了实验基础.     

Precision frequency measurement of ~1S_0–~3P_1 intercombination lines of Sr isotopes

We report on frequency measurement of the intercombination(5s2)1S0–(5s5p)3P1transition of the four natural isotopes of strontium,including88Sr(82.58%),87Sr(7.0%),86Sr(9.86%),and84Sr(0.56%).A narrow-linewidth laser that is locked to an ultra-low expansion(ULE)optical cavity with a finesse of 12000 is evaluated at a linewidth of 200 Hz with a fractional frequency drift of 2.8×10-13at an integration time of 1 s.The fluorescence collector and detector are specially designed,based on a thermal atomic beam.Using a double-pass acousto-optic modulator(AOM)combined with a fiber and laser power stabilization configuration to detune the laser frequency enables high signal-to-noise ratios and precision saturated spectra to be obtained for the six transition lines,which allows us to determine the transition frequency precisely.The optical frequency is measured using an optical frequency synthesizer referenced to an H maser.Both the statistical values and the final values,including the corrections and uncertainties,are derived for a comparison with the values given in other works.     

Ba0.98Bi0.02(Ti0.9Zr0.1)1-xCuxO3陶瓷的介电性能、弛豫行为与结晶化学特性

采用固相合成法,Bi3+作施主掺杂A位,Cu2+作受主掺杂B位,制备了Ba0.98Bi0.02(Ti0.9Zr0.1)1-xCuxO3(x=0,0.01,0.02,0.03)陶瓷样品。借助XRD、LCR等研究了该陶瓷的结构与介电性能。结果表明:当x=0.03时,陶瓷样品出现第二相。通过GULP模拟,缺陷偶极子的稳定性从低到高依次为:[2BiBa.+VBa″]、[2BiBa.+CuTi/Zr″]、[CuTi/Zr″+VO..],结合实验可知:介电弛豫程度与晶体中缺陷偶极子的存在形式相关,其中x=0.01时,晶体中以[2BiBa.+CuTi/Zr″]为主。随Cu2+掺杂量的增加,介电常数增加,介电常数与B位键价和呈反比变化、与八面体BO6的体积呈正比变化。     

莱茵衣藻(Chlamydomonas reinhardtii)cbn1和cao突变基因的对比分析及CAO基因的分子定位

用电击法将带有CAO基因片段的P sp109-E 8质粒转入到莱茵衣藻cbn1-48m t 基因突变株中后,转化子中出现了叶绿素b的恢复性表达,初步验证了丧失合成叶绿素b能力的cbn1和cao突变基因具有等位性的属性;将1641-1b(cbn1-43 m t )和CC-1354(cbn1-48 m t )突变株分别与CBS5(cao5 m t-)突变株的分离子CBS5-c1和CBS5-c5进行杂交,并通过随机分析方法分离获得1842个减数分裂后代分离子,经检测其中均没有发现有野生性表型的分离子,初步证明cbn1和cao 4突变基因间有着非常紧密的连锁性;从上述杂交系分离获得的50多个四分子中也没有检测发现显示野生性表型的分离子,进一步证明了cbn1和cao突变基因具有等位性的属性;根据CAO基因的DNA序列,从5′-端和3′-端设计两个探针,分别与莱茵衣藻核基因组Ⅰ号染色体上GBP 1和RB 47分子标记之间的21个BAC克隆进行的点杂交实验结果显示,该两个探针序列与21号BAC克隆(莱茵衣藻BAC文库序列号33e2)片段均有同源区的特性,此项DNA杂交实验初步证明,CAO基因的位点是在cbn1突变基因左右两侧的GBP 1和RB 47两个分子标记之间的33e2 BAC克隆片段区.