5—（4—氯苯基偶氮）—8—本磺酰氨基喹啉与钴（Ⅱ）的显色反应及其应用

本文用光度法研究了新显色剂 5 - (4-氯苯基偶氮 ) - 8-苯磺酰氨基喹啉 (CPBSQ)与钴的显色反应和最佳条件。结果表明 ,在 p H 9.5— 11.5范围内及有氯化十六烷基吡啶 (CPC)和硫脲 -酒石酸钾钠存在下 ,Co( )与 CPBSQ形成 1∶ 3的稳定配合物 ,其最大吸收波长为 5 90 nm。依此建立了一种测定 Co( )的新光度法。 Co( )的浓度在 0— 15 .0 μg/2 5 m L 范围内符合比耳定律 ,其摩尔吸光系数为 1.15× 10 5L·mol-1·cm-1。常见离子对 Co2 + 的测定均无严重干扰。本法具有灵敏度高、选择性好的特点。用于 VB12针剂中钴含量的测定 ,相对标准偏差为 0 .5 %— 0 .6 % ,标准加入回收率为 98%— 10 4 %。     

镍(Ⅱ)、锰(Ⅱ)、钴(Ⅱ)与诺氟沙星配合物的荧光特性研究

荧光分光光度法研究了镍(Ⅱ)、锰(Ⅱ)、钴(Ⅱ)与诺氟沙星配合物的荧光光谱特性.发现镍(Ⅱ)、锰(Ⅱ)、钴(Ⅱ)与诺氟沙星产生的配合物在pH 6.0的KH2PO4-K2HPO4的缓冲溶液中均使诺氟沙星的荧光猝灭.确认镍(Ⅱ)、锰(Ⅱ)、钴(Ⅱ)与诺氟沙星产生的配合物的组成分别为2 : 1、1:1、1:1.用锰与诺氟沙星配合物体系测定诺氟沙星滴眼液的含量,相对标准偏差为0.60%-1.1%,回收率为98.87%-102.7%,结果令人满意.     

钴(Ⅱ)与5-(5-碘-2-吡啶偶氮)-2,4-二氨基甲苯体系的络合物吸附波研究及应用

在pH为8.0的NaH2PO4-Na2HPO4缓冲溶液中,钴(Ⅱ)-NH2OH·HCl-5-(5-碘-2-吡啶偶氮)-2,4-二氨基甲苯(5-I-PADAT)体系在-1.25V(vs.SCE)产生—灵敏的络合物吸附波.据此建立了极谱法测定微量钴的新方法,该波一阶导数峰电流与钴(Ⅱ)的质量浓度在1-25μg·L-1范围内呈的线性关系,检出限达0.12μg·L-1.研究了该体系的极谱波性质,结果表明该波为催化吸附波,其电极过程为不可逆过程,电子转移数为2.此外还实验了多种离子对峰电流I′p的影响,所拟方法用于维生素B12注射液和陕南镍矿中微量钴的测定,结果满意.     

显色剂1-(2-苯并噻唑)-3-(5,7-二溴-8-喹啉)-三氮烯的合成及与钴的显色反应

合成了新显色剂 1- (2 -苯并噻唑 ) - 3- (5 ,7-二溴 - 8-喹啉 ) -三氮烯 (BTDBQT) ,并研究了在阳离子表面活性剂存在下与钴的显色反应。在 p H9.5— 10 .5的硼酸盐缓冲介质中 ,钴与该试剂形成 1∶ 2的蓝色铬合物 ,其最大吸收波长在 6 42 nm处 ,表观摩尔吸光系数为 1.0 5× 10 5L· mol-1·cm-1,钴 ( )的浓度在0— 2 4 0 μg/ L范围内符合比耳定律。显色反应具有良好的选择性 ,常见离子除铜、镍外 ,基本不干扰测定。已应用于维生素 B12 和水系沉积物中微量钴的测定     

5-(4-氯苯基偶氮)-8-苯磺酰氨基喹啉分光光度法测定微量镍(Ⅱ)

在 p H10 .5的 Na2 B4O7- Na OH介质及 CS(NH2 ) 2 、氯化十六烷基吡啶 (CPC)存在时 ,室温下镍 ( )与5 - (4 -氯苯基偶氮 ) - 8-苯磺酰氨基喹啉 (CPBSQ)反应 ,生成络合比为 1∶ 4的有色络合物 ,其最大吸收波长位于 6 0 0 nm。研究了反应的最佳条件 ,建立了一个测定 Ni( )的光度分析新方法。 Ni( )的浓度在 0—10 .0 μg/2 5 m L范围内符合比耳定律 ,其摩尔吸光系数为 1.93× 10 5L· mol-1·cm-1。考察了 2 0多种共存离子的影响 ,大多数常见离子在氨水沉淀分离后不干扰测定。方法用于合金钢中镍的测定 ,其相对标准偏差为 1.9%— 2 .1% ,标准加入回收率为 97%— 10 4 %。     

1-(8-喹啉)-3-(2-苯并噻唑)三氮烯(QBTT)分光光度法测定微量钯(Ⅱ)

研究了新显色剂 1 - (8-喹啉 ) - 3- (2 -苯并噻唑 )三氮烯 (QBTT)分光光度法测定 Pd( )的条件。在 p H1 1 .0的 Na2 B4O7- Na OH缓冲介质 ,该试剂与 Pd( )形成摩尔比为 2∶ 1的绿色稳定络合物。其最大吸收波长在 6 40 nm处 ,表观摩尔吸光系数 ε为 7.85× 1 0 4L·mol-1 ·cm-1 ,Pd( )的浓度在 0— 1 .2 μg/ m L范围内符合朗伯 -比尔定律。对 30多种共存离子的影响实结果表明 ,大多数常见离子不干扰测定。方法具有较好的选择性 ,用其直接测定催化剂样品中的微量钯 ,结果满意     

电感耦合等离子体-原子发射光谱法测定新锆合金(锆-锡-铁-铬-铌)中10种微量杂质元素

IPC-AES测定了新锆合金中10种微量杂质元素Al、Co、Cu、Mg、Mn、Mo、Ni、Pb、Ti和V.试液浓度为10mg/mL时,测定范围在20-1060μg/g之间,回收率在94%-108%之间,相对标准偏差(RSD,n=6)为4.3%-7.4%之间.     

新显色剂3,5-二(1-羧基-4,5-二甲氧基-2-苯氨基偶氮基)苯甲酸与铜(Ⅱ)的显色反应

研究了新显色剂3,5-二(1-羧基-4,5-二甲氧基-2-苯氨基偶氮基)苯甲酸(CDMOBAABA)与铜(Ⅱ)的显色反应。在TritonX-100存在下,于pH9.5的NH3-NH4Cl缓冲介质中,CDMOBAABA与铜(Ⅱ)形成棕红色配合物。试剂与络合物的最大吸收波长分别为450nm和540nm。表观摩尔吸光系数为2.43×105L·mol-1.cm-1。铜(Ⅱ)含量在0—20μg/25mL范围内符合比耳定律。该方法用于铝合金样品中铜的测定,结果与原子吸收光谱法相吻合,相对标准偏差1.89%。     

2,6-二(苯并咪唑-2′)吡啶与钴(Ⅱ)的显色反应

在 (CTMAB)存在下 ,在 p H =3.5— 4 .5的 HAc- Na Ac缓冲溶液中 ,2 ,6 -二 (苯并咪唑 - 2′)吡啶(H2 Bzimpy)与钴 ( )形成稳定的 3∶ 1配合物 ,其最大吸收波长为 36 0 .6 nm,表观摩尔吸光系数为 4 .4 6 7× 1 0 4L· mol-1 · cm-1 ,钴 ( )的质量浓度在 0— 2 0μg/ 2 5 m L范围内服从比耳定律。该法用于维生素 B1 2 和含钴分子筛中微量钴的测定 ,结果令人满意     

二阶导数光谱-峰面积积分法同时测定芦荟中痕量铁(Ⅱ)和钴(Ⅱ)

在 1,10 -邻菲罗啉显色体系中 ,引入二阶导数光谱 -峰面积积分技术 ,建立了同时测定痕量铁 ( )和钴 ( )的新方法。该法可有效消除共存离子的干扰 ,提高了准确度和灵敏度。对铁和钴的表观摩尔吸光系数分别为 εFe5 .4 5× 10 6 L·mol-1·cm-1,εCo 1.1× 10 4 L· mol-1· cm-1;铁含量在 0 .0— 8.5 μg·m L-1,钴含量在 0 .0— 7.3μg· m L-1范围内遵守比耳定律。可用于芦荟中铁和钴的同时测定 ,结果令人满意     

Search for the lepton-number-violating decay Xi(-)-->pmu(-)mu(-)

A sensitive search for the lepton-number-violating decay Xi(-)-->pmu(-)mu(-) has been performed using a sample of approximately 10(9) Xi(-) hyperons produced in 800 GeV/c p-Cu collisions. We obtain B(Xi(-)-->pmu(-)mu(-))<4.0x10(-8) at 90% confidence, improving on the best previous limit by 4 orders of magnitude.     

1-(4-安替比林)-3-(8-喹啉)-三氮烯的合成及其分析应用

报道了新试剂1-(4-安替比林)-3-(8-喹啉)-三氮烯(APQT)的合成及其与镉(Ⅱ)的显色反应研究.在Triton X-100存在下,pH 10.5的Na2B4O7-NaOH的缓冲溶液中,试剂与镉(Ⅱ)形成2:1型的橙红色络合物,最大吸收波长为525nm,表观摩尔吸光系数为2.25×105L·mol-1·cm-1,镉含量在0-15μg/25mL范围内遵守比耳定律.     

Polyethylene glycol (PEG-400) promoted one-pot,five-component synthesis of (E)-ethyl2-(2-((E)-2-(1-(4-methyl-2-(phenylamino)thiazol-5yl)ethylidene)hydrazinyl)-4-oxothiazol-5(4H)-ylidene)acetates

Molecular Diversity - A facile, inexpensive and eco-friendly synthesis of functionalised...     

Search for the lepton-flavor-violating leptonic B(0)-->mu(+/-)tau(-/+) and B(0)-->e(+/-)tau(-/+)

We have searched a sample of 9.6 x 10(6) BB events for the lepton-flavor-violating leptonic B decays, B(0)-->mu(+/-)tau(-/+) and B(0)-->e(+/-)tau(-/+). The tau lepton was detected through the decay modes tau-->lnunu(-) , where l=e, mu. There is no indication of a signal, and we obtain the 90% confidence level upper limits B(B(0)-->mu(+/-)tau(-/+))<3.8 x 10(-5) and B(B(0)-->e(+/-)tau(-/+))<1.3 x 10(-4).     

Ground- and excited-state spectroscopic studies on [1-(4-methoxyphenyl)-3-(amino)-2,4-(dicyano)-9,10-tetrahydrophenanthrene]

The effects of polar and nonpolar solvents on both the ground and the excited-state properties of [1-(4-methoxyphenyl)-3-(amino)-2,4-(dicyano)-9,10-tetrahydrophenanthrene] is examined. Light absorption results in a population of a locally excited (LE) first singlet state (S₁,n^*) which shows sensitivity to the polarity of the surrounding solvent and hydrogen-bonding ability to the quencher 4-methylpyridine. Relaxation of this state leads to an intramolecular charge-transfer state (ICT) which leads to a large Stokes shift in polar solvents and an excited-state dipole moment of _e= 10D. The quenching of the fluorescence state by 4-methylpyridine studied inn-hexane and acetonitrile at room temperature is found to be efficient and a positive deviation from linearity was observed in the Stern-Volmer plots even at concentrations of 4-methylpyridine below 0.4M. This is explained as a result of the occurrence of both a dynamic and a static quenching mechanism. The static quenching constants (K _sv) along with those obtained by visible spectroscopy (K _GS) indicate that the ground-state complex is weak and relatively solvent dependent.     

Search for the lepton family number violating process nu(mu)e(-) --> mu(-)nu(e)

The NuTeV experiment at Fermilab has used a sign-selected neutrino beam to perform a search for the lepton number violating process nu(mu)e(-)-->mu(-)nu(e), and to measure the cross section of the standard model inverse muon decay process nu(mu)e(-)-->mu(-)nu(e). NuTeV measures the inverse muon decay asymptotic cross-section slope sigma/E to be (13.8 +/- 1.2 +/- 1.4) x 10(-42) cm(2)/GeV. The experiment also observes no evidence for lepton number violation and places one of the most restrictive limits on the cross-section ratio sigma(nu(mu)e(-)-->mu(-)nu(e))/sigma(nu(mu)e(-)-->mu(-)nu(e)) < or = 1.7% at 90% C.L. for V-A couplings and < or = 0.6% for scalar couplings.     

新型锌离子荧光探针(5-(二甲基氨基)-N-(4-(2-(2-喹啉亚甲基)甲酰肼基)苯基)萘-1-磺酰胺)的研究

以丹磺酰胺为荧光基团设计合成了新型Zn²⁺荧光探针DW1(5-(二甲基氨基)-N-(4-(2-(2-喹啉亚甲基)甲酰肼基)苯基)萘-1-磺酰胺)。通过紫外光谱、荧光光谱及电喷雾质谱研究了DW1对Zn²⁺的选择性识别作用。结果表明,DW1与Zn²⁺结合后荧光显著增强,荧光发射光谱由545 nm蓝移至515 nm,量子产率达到0.32,且对Zn²⁺具有较高的选择性,受常见离子的干扰较小。光谱滴定和ESI-MS谱表明DW1与Zn²⁺以1∶1的化学计量数形成配合物,平衡常数K=1.75×10⁴(mol/L)^-1。     

Synthesis of( E ) -5- ( dimethylamino ) -N- ( 4- ( 2- ( quinolin-2-ylmethylene ) -hydrazinecarbonyi ) phenyl ) naphthalene-1-sulfonamide for Detection of Zinc Ion

以丹磺酰胺为荧光基团设计合成了新型Zn2+荧光探针DW1(5-(二甲基氨基)-N-(4-(2-(2-喹啉亚甲基)甲酰肼基)苯基)萘-1-磺酰胺).通过紫外光谱、荧光光谱及电喷雾质谱研究了DW1对Zn2+的选择性识别作用.结果表明,DW1与Zn2+结合后荧光显著增强,荧光发射光谱由545nm蓝移至515nm,量子产率达到0.32,且对Zn2具有较高的选择性,受常见离子的干扰较小.光谱滴定和ESI-MS谱表明DW1与Zn2+以1:1的化学计量数形成配合物,平衡常数K=1.75×104(mol/L)-1.     

Isotope fractionation in aqua-gas systems: Cl(2)-HCl-Cl(-), Br(2)-HBr-Br(-) and H(2)S-S(2-)

We report calculated values of isotope fractionation factors between chlorine, bromine and sulphide hydrated anions and respective gaseous compounds: hydrogen chloride, hydrogen bromide, molecular chlorine and bromine and hydrogen sulphide. For the calculation of the reduced partition function ratios (β-factors) of hydrated Cl(-), Br(-) and S(2-) anions, we used a model of a cluster composed of the considered ion surrounded by two shells of H(2)O molecules. Only the electrostatic interaction between ion and water molecules treated as electric dipoles was taken into account. The β-factors for the gaseous compounds (HCl, Cl(2), HBr, Br(2) and H(2)S) were calculated from vibrational frequencies reported by Urey and Greiff [Isotopic Exchange Equilibria, J. Am. Chem. Soc. 57, 321 (1935)] and Schauble et al. [Theoretical Estimates Equilibrium Chlorine-Isotope Fractionation, Geochim. Cosmochim. Acta 67, 3267 (2003)]. Low-temperature isotope fractionation between chlorine-hydrated anion and hydrogen chloride attains 1.55-1.68‰ (this work), which is in good agreement with experimental data (1.4-1.8‰) [Z.D. Sharp, J.D. Barnes, T.P. Fischer and M. Halick, An Experimental Determination of Chlorine Isotope Fractionation in Acid Systems and Applications to Volcanic Fumaroles, Geochim. Cosmochim. Acta 74, 264 (2010)]. The predicted isotope fractionations for hydrated bromine and HBr, Br(2) gases are very small, 1000?ln α, do not exceed 0.8‰; thus, the expected variations of bromine isotope composition in aqua-gas systems will require enhanced precision for their detection. In contrast, the sulphur isotope fractionation between H(2)S( gas ) and S(2-) attains 6.0‰ at room temperature and drops nearly linearly to 3.1‰ at 350°C.     

Observation of the decay K- --> pi(-)mu(+)mu(-) and measurements of the branching ratios for K+/- --> pi(+/-)mu(+)mu(-)

Using data collected with the HyperCP (E871) spectrometer during the 1997 fixed-target run at Fermilab, we report the first observation of the decay K--->pi(-)mu(+)mu(-) and new measurements of the branching ratios for K+/--->pi(+/-)mu(+)mu(-). By combining the branching ratios for the decays K+-->pi(+)mu(+)mu(-) and K--->pi(-)mu(+)mu(-), we measure Gamma(K+/--->pi(+/-)mu(+)mu(-))/Gamma(K+/--->all) = (9.8+/-1.0+/-0.5)x10(-8). The CP asymmetry between the rates of the two decay modes is [Gamma(K+-->pi(+)mu(+)mu(-))-Gamma(K--->pi(-)mu(+)mu(-))]/[Gamma(K+-->pi(+)mu(+)mu(-))+Gamma(K--->pi(-)mu(+)mu(-))] = -0.02+/-0.11+/-0.04.