吖啶橙-PAR-钒(Ⅴ)能量转移荧光猝灭法的研究及分析应用

在pH 5.5的Na2HPO4-柠檬酸缓冲溶液中,吖啶橙（AO）与PAR-钒（Ⅴ）络合物之间发生有效的能量转移,使吖啶橙526 nm处的荧光猝灭,据此建立了能量转移荧光测定痕量钒的新方法。实验表明,在pH5.5的3.0×10^-5mol.L^-1AO-4.0 mg.L^-1PAR体系中,钒的含量c在0.12-0.5μg.mL^-1范围内与荧光猝灭强度ΔF呈良好线性关系,线性回归方程为ΔF=165.4c＋2.5,方法检出限为0.0045μg.mL^-1,相对标准偏差为0.6%。该荧光猝灭反应15 min内完全,其相对荧光强度在2.5 h内基本保持不变。用该方法测定生物样品中钒的含量,相对误差小于5%,结果满足痕量分析要求。     

吖啶橙-罗丹明B荧光共振能量转移猝灭法测定砷

研究了利用吖啶橙(AO)-罗丹明B(RB)共振能量转移荧光猝灭法测定痕量砷的方法。在λ_ex/λ_em=470/580 nm,0.016 mol·L-1 H₂SO₄溶液中,十二烷基苯磺酸钠(DBS)存在下,吖啶橙-罗丹明B能够发生有效的能量转移,使罗丹明B的荧光强度大大增强;在酸性条件下,砷与钼酸铵生成砷钼杂多酸使能量转移体系罗丹明B的荧光猝灭。利用吖啶橙-罗丹明B能量转移荧光猝灭法测定痕量砷,砷在0.01～0.25 mg·L-1范围内与罗丹明B荧光猝灭程度呈良好的线形关系,方法检出限为2.56 μg·L-1。该方法用于茶叶中痕量砷的测定,相对标准偏差为0.48%～0.64%,回收率为98%～103%,结果满意。     

茜素红S荧光猝灭法测定壳聚糖含量

在pH 5.0的NaAc-HAc缓冲液中壳聚糖对茜素红S的荧光强度具有明显的猝灭作用,且猝灭程度F0/F与加入的壳聚糖浓度成线性关系,据此建立一种测定壳聚糖含量的荧光猝灭法。确定了最佳测定条件,线性回归方程为F0/F=-0.438 37 0.436 27c(mg·L-1),线性范围为0-16.667 mg·L-1,r=0.996,检测限为0.473 mg·L-1;平均回收率为100.60％,测定了样品中壳聚糖的含量,并考察了干扰因素对测定的影响。采用该方法可测定复杂样品中微量壳聚糖含量。     

吖啶橙-罗丹明6G能量转移荧光猝灭法测定维生素B12

研究了吖啶橙(AO)与罗丹明6G(R6G)间发生能量转移的最佳条件,在pH5·0的Na2HPO4-柠檬酸缓冲溶液,十二烷基苯磺酸钠介质中,AO-R6G间发生有效能量转移,使R6G荧光大大增强。维生素B12(VB12)的加入使AO-R6G体系的荧光猝灭,以此建立了利用AO-R6G能量转移荧光猝灭法测定维生素B12的新方法。在优化的实验条件下,维生素B12工作曲线的线性范围为:0~3·0×10-5mol·L-1;检出限为:4·8×10-7mol·L-1;平行6次测定相对标准偏差为0·51%~0·64%;回收率为98·40%~103·62%。该方法的稳定性好,选择性高,用于维生素B12注射液中维生素B12含量的测定,结果满意。     

邻羟基苯基荧光酮荧光法测定牛血清白蛋白

研究了邻羟基苯基荧光酮(o-HPF)荧光光度法测定牛血清白蛋白(BSA)的反应条件,在pH 7.90的BR缓冲溶液中,o-HPF与BSA作用形成稳定的结合物,导致体系荧光猝灭,依据其荧光猝灭程度与外加BSA量的关系建立了定量测定BSA的方法.该方法具有良好的选择性和稳定性,实验操作简单,干扰少,灵敏度较高,测定BSA线性范围为1.32～18.54μg·mL-1,回归方程为△F=431.51c(10-7 mol·L-1) 457.78,相关系数,r=0.997.测定方法中重金属离子如Pb(Ⅱ)等对BSA测定允许量较低,其他物质的存在对BSA的测定干扰较小.通过对o-HPF与BSA作用荧光猝灭常数的测定及热力学常数计算,讨论了o-HPF与BSA的作用机理,表明o-HPF与BSA作用方式主要为静电引力的非共价作用,BSA对o-HPF荧光猝灭为分子间形成了结合物而引起的静态猝灭.     

N-(1-萘基)-乙二胺荧光光度法测定痕量亚硝酸根

研究了盐酸介质中N-(1-萘基)-乙二胺(NED)与亚硝酸根的反应。基于NED的荧光强度被亚硝酸根猝灭的现象,建立了一种荧光测定NO-₂的新方法,并对反应机理进行了讨论。在优化实验条件下,NO-₂在1.07～214.0 μg·L-1范围内与NED的荧光猝灭强度呈线性关系,方法的检出限为0.069 μg·L-1。该法用于测定水样中痕量亚硝酸根的含量,结果令人满意。     

5-溴水杨基荧光酮-曲拉通x-100-羟丙基-β-环糊精荧光猝灭法测定痕量锰

在羟丙基-β-环糊精(HP-β-CD)和曲拉通X-100(Triton X-100)存在下,以NaAc-HAc缓冲溶液为介质,5-溴水杨基荧光酮(5-BrSAF)为荧光试剂,建立了用荧光猝灭法测定痕量锰的新方法.研究了缓冲溶液、显色剂用量、表面活性剂对体系的影响,确定了最佳实验条件.体系的最大激发波长λex=375nm,最大发射波长λex=535nm,Mn2+含量在0.026-3.5μg/25mL范围内与荧光猝灭值△F呈线性关系,方法检出限为1.02μg/L.已用于面粉中锰的测定.     

基于NaGdF_4∶Eu纳米粒子的荧光猝灭测定痕量Cu~(2+)

采用水热法合成了柠檬酸盐修饰的水溶性NaGdF4:Eu荧光纳米粒子,粒子溶液荧光强度稳定.实验发现,Cu2+外对合成粒子的荧光有猝灭作用,据此可建立用NaGdF4:Eu荧光探针测定痕量Cu2+的新方法.实验确定NaGdF4:Eu的浓度为1.0×10-3 mol·L-1,溶液的pH值为10.0.考察了其他常见离子对粒子荧光性能的影响,其中Fe3+使荧光发生猝灭,用三乙醇胺可消除Fe3+的干扰.标准曲线的线性回归方程为I=532-0.685c,相关系数r为-0.998 4,线性范围为3.33×10-6～1.33×10-4 mol·L-1,检出限为8.9×10-7 mol·L-1,对浓度为6.0×10-5 mol·L-1的Cu2+溶液平行测定11次,RSD为0.62%.以上结果表明,方法的线性范围较宽,灵敏度和精密度较高.测定了茶叶样品中铜含量,测定结果和原子吸收法测定结果相一致.分析Cu2+对粒子荧光猝灭的机理认为,Cu2+和粒子表面的柠檬酸根发生化学结合,改变了粒子表面的结构和组成,导致其荧光发生猝灭.     

PAR-吖啶黄能量转移荧光猝灭法测定痕量铁(Ⅱ)的研究

对 4 (2 吡啶偶氮 ) 间苯二酚 (PAR)与吖啶黄间荧光能量转移进行了探讨 ,研究了其能量转移的最佳条件 ,并应用该体系测定痕量铁 (Ⅱ ) ,由此建立了能量转移荧光测定痕量铁的新方法。在λex/em =46 5nm/5 0 5nm ,十二烷基硫酸钠 (SDS)作用下 ,pH =9 2时 ,吖啶黄与PAR 铁 (Ⅱ )络合物间能发生有效能量转移 ,使吖啶黄的荧光猝灭。铁的量在 0～ 10 μg·L-1范围内呈良好的线性关系。最低检出限 0 0 6 μg·L-1。该方法用于水样、发样中痕量铁的测定 ,结果满意。     

壳聚糖包覆的CdTe量子点荧光猝灭法测定吉米沙星

以壳聚糖包覆的CdTe量子点为荧光探针,基于荧光猝灭法建立了吉米沙星定量测定方法。结果表明,体系的荧光强度与吉米沙星浓度在3.46×10-9～3.46×10-7 g.L-1范围内呈良好的线性关系(r=0.999 2),线性回归方程为F0/F=1.063 7+0.016 7c(g.L-1)。对2.77×10-7 g.L-1吉米沙星溶液进行7次平行测定的相对标准偏差为2.7%,基于荧光猝灭法相关理论证明了该相互作用过程为静态猝灭。本方法灵敏度高,检测线性范围宽,为吉米沙星定量测定提供了简便可靠的方法。     

Theoretical Study of the Collision-Induced Double Transition CO(2) (nu(3) = 1) + N(2) (nu(1) = 1) <-- CO(2) (nu(3) = 0) + N(2) (nu(1) = 0) at 296 K

A procedure is presented for the calculation of the double vibrational collision-induced absorption CO(2) (nu(3) = 1) + N(2) (nu(1) = 1) <-- CO(2) (nu(3) = 0) + N(2) (nu(1) = 0) on the basis of quantum lineshapes computed using an isotropic potential and dipole-induced dipole functions. The linestrengths and energies of the vibration-rotation transitions are treated explicitly for N(2), utilizing the HITRAN database for CO(2). The theoretical absorption profile is compared to recent experimental results. By narrowing the width of the individual lines contributing to the overall absorption profile relative to their values determined for N(2)-N(2) collision-induced absorption, excellent agreement between theory and experiment is obtained. Copyright 2000 Academic Press.     

First Observation of the nu(17)-nu(4) Difference Bands of Diborane (10)B(2)H(6) and (11)B(2)H(6)

An analysis of the nu(17)-nu(4) difference bands near 800 cm(-1) of two isotopic species, (10)B(2)H(6) and (11)B(2)H(6), of diborane has been carried out using infrared spectra recorded with a resolution of ca. 0.003 cm(-1). In addition, the nu(17) band of (10)B(2)H(6) has been recorded and assigned. Since this band in (11)B(2)H(6) had already been studied (R. L. Sams, T. A. Blake, S. W. Sharpe, J.-M. Flaud, and W. J. Lafferty, J. Mol. Spectrosc. 191, 331-342 (1998)), it was possible to derive precise energy levels and Hamiltonian constants for the 4(1) vibrational states of both isotopic species. Copyright 2000 Academic Press.     

The 2(3)Delta(g) State of (7)Li(2)

Using pulsed perturbation-facilitated optical-optical double resonance (PFOODR) spectroscopy, the 2(3)Delta(g) state of (7)Li(2) (electronic configuration (varsigma(g)2s) (4ddelta(g)), effective principal quantum number n* = 4.101) has been observed and assigned. Molecular constants and a RKR potential energy curve were obtained. The major molecular constants are Copyright 2000 Academic Press.     

The Perturbation between the G(1)Pi(g) and 2(1)Delta(g) States of (7)Li(2)

We have observed the rotational levels in the v = 2, 3, 5, 6, 7, and 8 vibrational manifolds of the 2(1)Delta(g) state of (7)Li(2) via the A(1)Sigma(+)(u) intermediate levels by DeltaLambda = 2 transitions. This violation of the DeltaLambda = 0, +/-1 selection rule is due to the interaction with the G(1)Pi(g) state. Band-by-band deperturbations of the G(1)Pi(g) approximately 2(1)Delta(g) (v(Pi), v(Delta)) = (11, 2), (12, 3), (15, 5), (16, 6), (18, 7), and (19, 8) bands have been performed. Deperturbed molecular constants and rotational-electronic interaction parameters are reported here. Copyright 2000 Academic Press.     

Rovibrational Intensities of the (00(0)3) <-- (10(0)0) Dyad Absorption Bands of (12)C(16)O(2)

Absolute line intensities of (12)C(16)O(2) are experimentally measured for the first time for the (00(0)3)(I) <-- (10(0)0)(II) band at 5687.17 cm(-1) and the (00(0)3)(I) <-- (10(0)0)(I) band at 5584.39 cm(-1). The spectra were obtained using a Bomem DA8 Fourier transform spectrometer and a 25-m base-path White cell at NASA-Ames Research Center. The rotationless bandstrengths at a temperature of 296 K and the Herman-Wallis parameters are S(0)(vib) = 6.68(30) x 10(-25) cm(-1)/(molecule/cm(2)); A(1) = 1.4(9) x 10(-4), and A(2) = -1.1(5) x 10(-5) for the (00(0)3)(I) <-- (10(0)0)(II) band and S(0)(vib) = 6.07(22) x 10(-25) cm(-1)/(molecule/cm(2)); A(1) = 5.2(1.5) x 10(-4) and A(2) = -4.0(7) x 10(-5) for the (00(0)3)(I) <-- (10(0)0)(I) band.     

The v(1)+v(3) Bands of the (16)O(17)O(16)O and (16)O(16)O(17)O Isotopomers of Ozone

Using 0.002 cm(-1) resolution Fourier transform absorption spectra of an (17)O enriched ozone sample, an extensive analysis of the v(1)+v(3) bands of the (16)O(17)O(16)O and (16)O(16)O(17)O isotopomers of ozone has been performed for the first time. The experimental rotational levels of the (101) vibrational states were satisfactorily reproduced using a Hamiltonian matrix that takes into account the observed rovibrational resonances. More precisely, for (16)O(17)O(16)O, as for the other C(2v)-type ozone isotopomers, it was necessary to account for the Coriolis type resonances linking the (101) rotational levels with the levels of the (200) and (002) vibrational states and the Darling-Dennison interaction coupling the levels of (200) with those of (002). For the C(s)-type isotopomer, namely (16)O(16)O(17)O, as for (16)O(16)O(18)O and (16)O(18)O(18)O, it proved necessary to also account for an additional DeltaK(a)&equals+/-2 resonance involving the rotational levels from (101) and (002) (J.-M. Flaud and R. Bacis, Spectrochimica Acta Part A 54, 3-16 (1998)). Using a Hamiltonian matrix which takes these resonances explicitly into account, precise vibrational energies and rotational and coupling constants were deduced, leading to the following band centers: v(0)(v(1)+v(3))=2078.3496 cm(-1) for (16)O(17)O(16)O and v(0)(v(1)+v(3))=2098.8631 cm(-1) for (16)O(16)O(17)O. Copyright 2001 Academic Press.     

CO2同位素分子16O12C16O, 16O12C17O, 16O13C17O配分函数研究

本文主要研究了CO2的三种同位素分子16O12C16O , 16O12C17O ,16O13C17O 70 K~6000 K的总内配分函数 (TIPS)。在总内配分函数的计算中, 转动配分函数的计算采用了McDowell的解析式法, 振动配分函数则采用了简谐振动近似(HOA)获得。最后通过将两配分函数乘积近似计算得出TIPS, 并将其70~3000 K的数据和HITRAN04数据进行了比较, 发现所得结果和数据库符合的较好, 且其误差可以近似看成一条直线。并通过对误差的拟合修订了高温区(3000~6000 K)的计算数据, 给出了在高温下的较为准确的TIPS值。     

Torsional Splitting in the nu(5) Fundamental Infrared Band of CH(3)CD(3) and (13)CH(3)CD(3)

The nu(5) fundamental (C-C stretching) of CH(3)CD(3) shows a resolved torsional structure, caused by perturbations due mainly to the linear dependence of the torsional potential barrier on the normal coordinate Q(5). We were able to analyze this structure and to assign vibration-rotation transition wavenumbers for all five torsional components, classified according to the symmetry species of the G(18)((3)) extended molecular group. The torsional splitting pattern is qualitatively similar to that of a nondegenerate vibrational state with an even number of excited torsional quanta v(6). Explorative calculations show that the main perturber system should consist of the torsional components of the vibrational ground state correlating with v(6)=4 in the high barrier limit. The strength of the perturbation on the E(r0) torsional components of nu(5) increases rapidly with r, the E(40) component being the most affected. The observed transition wavenumbers can be reasonably fitted by a simplified model containing independent effective vibration-rotation parameters for the five different torsional components of nu(5), for both CH(3)CD(3) and (13)CH(3)CD(3). The trend of the determined values of the effective vibrational wavenumbers and rotational parameters over the torsional components supports the proposed vibration-torsion interaction mechanism, responsible for the observed torsional splittings. A strong anomaly observed in the rotational intensity distribution of nu(5) is discussed. Copyright 2001 Academic Press.