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1.
研究了DNA与铜(Ⅱ)-L丝氨酸-二吡啶并[3,2-a:2',3'-c]吩嗪配合物[Cu(DPPZ)(L-Ser)-]+相互作用的共振光散射光谱和紫外可见吸收光谱,通过研究体系与溴化乙啶相互作用的荧光光谱特征,证明其作用方式为插入作用.在pH 7.2的缓冲溶液中,[Cu(DPPZ)(L-Ser)]+由于插入作用而在DNA表面聚集,使体系的共振光散射强度增强,最大敞射峰在400 nm处.在最佳实验条件下,共振光散射增强的强度与浓度在0.42~4.20 ng·mL1范围的DNA具有良好的线性关系.方法的检出限为0.29 ng·mL-1.该法用于DNA样品的测定,回收率在97.8%~106.0%之间.  相似文献   

2.
研究了罗丹明6G(R6G)的荧光光谱、共振散射光谱和吸收光谱,讨论了共振光散射与共振荧光的区别与联系。在罗丹明6G水溶液的三维荧光等高线光谱中,瑞利散射线与荧光等高线有部分相交。共振散射峰(544nm)介于荧光激发峰(530nm)和发射峰(552nm)之间。由光偏振实验,测得R6G共振散射光谱544nm处的偏振度P为0.0105。上述实验结果证明,R6G的共振散射峰主要是共振荧光。共振光散射信号随pH值增大而增强的机理是R6G酸碱平衡移动导致荧光型体的形成。由于自吸收的影响,荧光强度、共振散射光强度与R6G浓度之间不是严格的线性关系。  相似文献   

3.
罗丹明B的共振散射光谱研究   总被引:8,自引:0,他引:8  
研究了罗丹明B(RhB)的共振光散射的特性与机理。在 pH =- 0 38至 pH 4 10的酸性溶液中 ,共振光散射信号随pH值增大而增强 ,近中性时散射强度达到最大。散射强度随波长的变化不符合瑞利散射定律。RhB的荧光激发光谱与发射光谱有部分重叠 ,共振散射峰处于荧光激发峰和荧光发射峰之间。在三维荧光等高线光谱图中 ,瑞利散射线与荧光等高线相交。在光偏振实验中 ,测得共振散射光的偏振度P≈ 0 1。上述实验结果揭示RhB的共振散射光主要是共振荧光。共振光散射信号随 pH值增大而增强的机理是RhB酸碱平衡移动导致荧光型体的形成。RhB的共振散射峰位于吸收曲线轮廓之中 ,共振光散射受光吸收的影响 ,因此 ,散射光强度与浓度之间不是严格的线性关系。  相似文献   

4.
在pH 为4.6的HAc-NaAc介质中,盐酸巴马汀与桑色素通过静电引力发生反应,得到具有疏水性的离子缔合物,致使体系在308 nm处的共振光散射信号显著增强。研究表明,体系增强的共振光散射信号强度与盐酸巴马汀的浓度在0.08~1.0 μmol·L-1之间具有良好的线性关系,检测限为8.0 nmol·L-1。由此建立了用于盐酸巴马汀检测的共振光散射分析方法。研究了体系的散射光谱和吸收光谱,通过扫描电镜和动态光散射考察离子缔合物的聚集情况并研究了体系的反应机理,研究了酸度及离子强度对体系的影响,最终实验选择pH 4.6的HAc-NaAc缓冲,不加NaCl控制体系离子强度的情况下信号最佳。探讨了体系的稳定性,结果显示本反应体系反应迅速,5min内散射强度即可达到最大值并至少能稳定120 min。考察了可能存在的共存物质的影响,结果发现常见的金属离子,无机阴离子,部分糖类及氨基酸不影响对盐酸巴马汀的检测。该方法具有简单,快速,灵敏度高的优点。该法成功用于实际药片和胶囊中盐酸巴马汀含量的测定,RSD≤3.3%。  相似文献   

5.
研究了抗癌药物阿霉素与DNA相互作用的吸收光谱、荧光光谱和共振光散射光谱,发现阿霉素与DNA相互作用产生强烈增强的共振光散射信号,共振光散射技术在研究DNA与阿霉素的相互作用时,其灵敏度远远高于吸收光谱和荧光光谱。DNA与阿霉素作用在322与564 nm处产生两个共振散射峰,在弱酸性条件下(pH 5.72),DNA的浓度在0~8.0 μg·mL-1范围内与散射强度呈良好的线性关系,对小牛胸腺DNA和鱼精子DNA的检出限分别为36.8和40.1 ng·mL-1。由此建立了一种选择性好,灵敏度高的DNA共振光散射分析方法。  相似文献   

6.
玫苯胺共振光散射法测定DNA   总被引:8,自引:1,他引:7  
本文研究了三苯甲烷类碱性染料玫苯胺与DNA作用的共振光散射光谱 ,在 pH =10 5~ 11的范围内 ,DNA的加入导致玫苯胺共振光散射的增强 ,在 4 85nm处 ,存在一共振光散射增强峰 ,其强度与DNA的浓度呈线性关系 ,据此建立了一种测定DNA的共振光散射法。方法的线性范围为 0~ 1 0 0mg·L-1,检测限为14 2ng·mL-1。将该方法用于混合样品中DNA的测定 ,结果令人满意。  相似文献   

7.
光谱法研究EGCG-Cu(Ⅱ)与ctDNA的相互作用   总被引:1,自引:1,他引:0  
研究了EGCG-Cu(Ⅱ)-ctDNA系统的荧光光谱,电子吸收光谱和共振光散射光谱(RLS)。与EGCG-Cu(Ⅱ)二元配合物比较,EGCG-Cu(Ⅱ)-ctDNA三元体系光谱显示以下特征:(1)荧光光谱的发射位置没有变,荧光强度显著增强,并且三元体系的荧光强度随着DNA浓度增大而增大。在适宜的条件下,Cu(Ⅱ)-EGCG 配合物有望成为检测ctDNA的荧光探针;(2)电子吸收光谱有明显的增色效应;(3)共振光散射强度也增强。三种光谱的特征显示,EGCG-Cu(Ⅱ)配合物与核酸之间主要依靠插入作用和静电引力结合。由于配合物的插入,使系统的荧光强度增强,而静电作用使其电子吸收光谱和共振光散射光谱产生增色效应。酸度和离子强度对三元系统荧光强度的影响也进行了实验和讨论。  相似文献   

8.
柯里拉京与DNA相互作用的光谱研究   总被引:1,自引:1,他引:0  
在p H 7.4的生理条件下,以溴化乙锭(EB)作为荧光探针,利用荧光光谱、紫外-可见吸收光谱、共振散射光谱法结合盐效应和DNA熔点(T_m)实验研究了柯里拉京(Cor)与小牛胸腺DNA分子之间的相互作用机制。实验结果表明,Cor静态猝灭DNA-EB体系的荧光。Cor与DNA作用后,其特征吸收峰强度发生减色效应;与DNA作用导致Cor在480.5 nm处的共振散射峰增强,并在330.2 nm处出现新共振散射峰。盐效应对Cor与DNA分子相互作用的影响较小。与Cor作用引起DNA的T_m值升高5.5℃。由此推断,Cor与DNA相互作用的主要方式为嵌插,两者间形成了超分子体系。通过计算获得Cor与DNA间结合常数(K_A)为5.82×10~3L/mol(298 K)、2.47×10~4L/mol(310 K),它们之间的作用为熵驱动的自发、吸热过程,疏水作用力是主要的非共价作用方式。  相似文献   

9.
新的光散射体系测定蛋白质的研究   总被引:1,自引:1,他引:0  
以1,6-己二胺二吖啶为荧光探针,建立了一种新的蛋白质共振散射检测体系。实验考察了该吖啶荧光探针的共振散射特征光谱、散射反应稳定性,研究了缓冲介质pH、探针浓度等参数对测定蛋白质的影响。结果表明,当pH 8.9时,1,6-己二胺二吖啶染料的散射波长为470 nm;加入BSA,反应约9 min后,体系光散射强度达到最大并维持稳定,2 h内无明显变化。当1,6-己二胺二吖啶探针(浓度1.00×10-4mol·L-1)用量为3.00 mL时,蛋白质与1,6-己二胺二吖啶的光散射增强作用显著,共振散射强度随着BSA的增加而明显增强,光散射强度与蛋白质浓度成良好线性关系,线性浓度范围为1.00~5.00 μg·mL-1,检测限(3σ/K)为0.085 μg·mL-1。测定了血清样品,浓度为2.00~4.00 μg·mL-1,回收率为98.0%~101.7%,测定偏差小于1.7%。  相似文献   

10.
甲苯胺蓝共振光散射法测定纳克级脱氧核糖核酸   总被引:15,自引:0,他引:15  
研究了吩噻嗪类染料甲苯胺蓝 (TB)与DNA作用的共振光散射光谱 ,在pH 1 0~ 1 1的范围内 ,加入DNA导致甲苯胺蓝共振光散射增强 ,在 35 0nm处 ,存在一共振光散射增强峰 ,其强度与DNA浓度呈线性关系 ,据此建立了一种测定DNA的共振光散射法。对于ctDNA ,方法的线性范围为 0~ 90 0ng·mL-1 ,检出限为6 75ng·mL-1 ,RSD为 3 7% ;对于fsDNA ,方法的线性范围为 0~ 90 0ng·mL-1 ,检出限为 2 99ng·mL-1 ,RSD为 5 6 % .已用于合成样品中DNA的测定  相似文献   

11.
The investigation was made of the dependence of the intensity of Tl, Ga, Mo, Mg, Mn, Sn, Bi, Ni, Zn, Pt and Au spectral lines and the plasma parameters (temperature T, electron concentration ne, degree of 6 ionnization α) from concentration of lithium additive.  相似文献   

12.
There is a tunnel connecting the beamcorridor and the target station in the spectrum hall in the CSNS project.The length of the tunnel is about 20 m.The shielding design of the tunnel is very significant for the persons working in the spectrum hall because the tunnel is not covered ed soil for shielding.In order to reduce the dose rate at the exit of the cable ducts,we use the ISIS construction,which is designed with four turnings,as a reference for the tunnel design.The thickness of the shielding is obtained by a simulationwith the Monte Carlo Code FLUKA.The result is compared with the data obtained with Moyer Mode and the reliability of the simulation is proved.This paper provides the basis for the design of the tunnel.  相似文献   

13.
There is a tunnel connecting the beamcorridor and the target station in the spectrum hall in the CSNS project. The length of the tunnel is about 20 m. The shielding design of the tunnel is very significant for the persons working in the spectrum hall because the tunnel is not covered by soil for shielding. In order to reduce the dose rate at the exit of the cable ducts, we use the ISIS construction, which is designed with four turnings, as a reference for the tunnel design. The thickness of the shielding is obtained by a simulation with the Monte Carlo Code FLUKA. The result is compared with the data obtained with Moyer Mode and the reliability of the simulation is proved. This paper provides the basis for the design of the tunnel.  相似文献   

14.
三棱镜折射率的测量是大学物理实验的重要组成部分,对培养学生的基本实验技能、加深对经典光学理论的理解具有重要作用。本文依据几何光学原理探究了最小偏向角法中在有出射光时最小偏向角与三棱镜顶角、折射率所对应的函数关系,建立了有出射光时入射角、折射率、顶角间以及最小偏向角时折射率、顶角、最小偏向角间的相图,阐明了两相图的物理意义。该研究拓展了三棱镜折射率实验的研究思路。  相似文献   

15.
范祖辉 《物理》2005,34(4):240-245
文章对微波背景辐射的各向异性、偏振及宇宙电离的历史给出了评述性介绍.从大爆炸理论的预言,到观测的发现,到其各向异性及偏振的探测,微波背景辐射(CMB)向人们揭示了丰富的宇宙学信息.文章在对基本理论作了简单介绍后,着重讲述了最新的CMB的观测结果及其物理意义.特别对微波背景各向异性探测器(Wilkinson Microwave Anisotropy Probe,WMAP)的偏振观测及其对宇宙重新电离的限制给出了较详细的叙述.  相似文献   

16.
Cosmologically stabilizing radion along with the dilaton is one of the major concerns of low energy string theory. One can hope that T and S dualities can provide a plausible answer. In this work we study the impact of S and T duality invariances on dilaton gravity. We have shown various instances where physically interesting models arise as a result of imposing the mentioned invariances. In particular S duality has a very privileged effect, in that the dilaton equations partially decouple from the evolution of the scale factors. This makes it easy to understand the general rules for the stabilization of the dilaton. We also show that certain T duality invariant actions become S duality invariance compatible. That is, they mimic S duality when the extra dimensions stabilize.  相似文献   

17.
In this paper, MgO film is successfully grown on polycrystalline and monocrystalline alumina substrates using sol-gel method, and polycrystalline and monocrystalline Mg-Al spinels are fabricated by solid state reaction, respectively. The influence of annealing temperature and time on the lattice structure and growth of the formed Mg-Al spinel layer has been investigated. It is indicated that the annealing temperature and time on the as-synthesized polycrystalline Mg-Al spinel has more significant influence than that of single crystal Mg-Al spinel. The thickness of the Mg-Al spinel layer increases with the annealing temperature, both for polycrystalline and for monocrystalline alumina substrates. And the significantly intercrystalline diffusion of Mg2+ ions and Al3+ ions results in a quicker growth velocity of the Mg-Al spinel layer than that of intracrystalline diffusion.  相似文献   

18.
The vibrational relaxation of OCl and OCl in the bulk and the liquid/vapor interface of water and acetonitrile is studied by molecular dynamics computer simulations. Both equilibrium calculations of the vibrational friction and non-equilibrium simulation of the energy relaxation are used to elucidate the factors that influence the rate of energy relaxation in systems that represent polar ionic and non-ionic solutes in polar protic and non-protic solvents. We find that, in agreement with previous experimental and theoretical studies, the relaxation of the ionic solute is much faster than that of the non-ionic solute in both the solvents. However, while the relaxation is slowed down considerably when the non-ionic solute is transferred from the bulk to the interface, no such surface effect is found in the case of the ionic solute. This behavior can be explained by noting that the ionic solute is able to keep its first solvation shell intact upon transfer to the interface and that the main contribution to the friction is due to the Lennard-Jones part of the intermolecular potential.  相似文献   

19.
20.
A model of symmetries and gauge interactions relating the electron and muon is considered. The model is based on the UL(1)?UR(1)?RL?RR group where UL(1)?UR(1) denotes the chiral e-μ rotation and RL?RR the chiral reflection of the electron field. The invariance under this group is spontaneously broken by the vacuum expectation values of scalar fields. A zeroth-order vacuum is found for which the zeroth-order electron mass vanishes, while one-loop corrections lead to a finite me ratio. The decay process μ → e + γ is strictly forbidden in this model.  相似文献   

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