在COIL中BHP的HO2－浓度对氯的利用率和激光功率的影响

 对COIL中碱性过氧化氢(BHP)溶液中的HO₂^-浓度进行了理论计算和实验测量,得到了HO₂^-浓度随不同浓度的KOH和H₂O₂以及不同比例（体积）配比的变化规律,并做了不同浓度HO₂^-对氯的利用率和激光输出功率影响的实验,获得的结果对优化BHP的配制和优化实验参数有较大的意义。     

Superacid Catalyst SO42-/ZrO2-La2O3 Prepared by Ultrasonic Co-precipitation and Low Temperature Aging

低温陈化超声波共沉淀法制得SO₄^2-/ZrO^2-La₂O₃前驱体, 经H₂SO₄处理, 在不同温度下焙烧得到纳米晶催化剂SO₄^2-/ZrO^2-La₂O₃;用Hammett指示剂法测定其酸性. 用XRD、BET、TEM、IR和XPS对样品进行表征,其催化活性用醋酸和甘油的酯化反应进行了评价. 结果表明经超声波搅拌和低温(-15 ºC)陈化,650 ºC焙烧4 h得到的固体超强酸表现出较高催化活性.     

由纳米管和纳米颗粒构成的TiO2膜的制备与机理研究

采用聚苯乙烯小球修饰Ti片表面,并进行阳极氧化,制备出一种由纳米颗粒和纳米管构成的TiO₂膜．通过数值模拟,分析了氧化表面附近的局部电场分布对TiO₂膜形貌的影响．结果表明,覆盖物增强了局部电场,从而加快了O^2-与Ti的反应速率,有利于TiO₂的生长;与此同时,[TiF₆]^6-的扩散受到阻碍,使得TiO₂的溶解速率减慢．可见,覆盖物打破了TiO₂纳米管形成的平衡条件,导致纳米颗粒的生成．此外,通过X射线衍射和Raman光谱的测试分析发现,所制备的TiO₂为锐钛矿结构.     

具有介孔结构的MnSiO3@Fe3O4@C纳米粒子的制备以及作为pH响应的T1-T2*双模MRI造影剂的研究应用

本文通过一个简单的、温和的方案制备了平均尺寸为120 nm,介孔结构的纳米粒子MnSiO₃@Fe₃O₄@C. 粒子的细胞毒性微小,可以用作T₁-T₂^*双模MRI造影剂. 酸性条件下MnSiO₃@Fe₃O₄@C释放出大量的Mn²⁺缩短T₁弛豫时间,提高成像分辨率. 超顺磁性的Fe₃O₄可以增强T₂对比成像,检测病变组织. 类似于肿瘤微环境/细胞器的酸性PBS(pH=5.0)中Mn²⁺的释放率达到31.66%,约为中性条件(pH=7.4)下的7倍. 释放的Mn²⁺通过内吞作用被细胞摄取,经肾脏排出,细胞毒性实验表明,MnSiO₃@Fe₃O₄@C具有低的细胞毒性,即使高浓度的200 ppm MnSiO₃@Fe₃O₄@C对HeLa细胞的毒性也相对较小. 对荷瘤小鼠静脉注射定量MnSiO₃@Fe₃O₄@C后,可以观察到一个快速增强的对比成像,给药24 h后,T₁MRI信号显著增强,达到132%,而T₂信号则明显降低至53.8%,活体MR成像证明了MnSiO₃@Fe₃O₄@C可以同时作为阳性和阴性造影剂. 此外,得益于介孔MnSiO₃优秀的酸敏感性,MnSiO₃@Fe₃O₄@C可以作为一种潜在的药物载体,实现肿瘤的诊疗一体化.     

焙烧温度对SiO2负载的Co3O4纳米粒子表面氧缺陷浓度和CO氧化催化性能的影响

以传统的浸渍法,在不同焙烧温度下制备了用于CO氧化反应的Co₃O₄/SiO₂催化剂．通过激光拉曼光谱(Raman)、X射线光电子能谱(XPS)、X射线衍射(XRD)、程序升温还原(TPR)和X射线吸收精细结构谱(XAFS)表征了该系列催化剂的结构．在所有的催化剂中,XRD和Raman光谱都只检测到了Co₃O₄晶相的存在．与Co₃O₄体相相比,XPS结果表明在200 oC焙烧的(Co₃O₄(200)/SiO₂)催化剂中Co₃O₄表面上存在着过量的Co²⁺．与XPS的结果一致,TPR结果表明Co₃O₄(200)/SiO₂催化剂中Co₃O₄表面上存在氧缺陷, 并且XAFS结果也表明Co₃O₄(200)/SiO₂催化剂中Co₃O₄具有更多的Co²⁺．提高焙烧温度使得过量的Co²⁺进一步氧化为Co³⁺,同时降低了表面氧缺陷浓度,从而得到计量比的Co₃O₄4/SiO₂催化剂．在所有的负载催化剂中Co₃O₄(200)/SiO₂催化剂表现出了最好的CO氧化催化性能,表明过量Co²⁺和表面氧缺陷的存在能够促进Co₃O₄催化CO氧化反应的活性.     

Sr2CeO4电荷迁移发光的光谱结构规律研究

利用高温固相反应法分别合成了不同物相形成机理的Sr₂CeO₄，Sr ₂CeO₄∶Ca ²⁺和Sr₂CeO₄∶Ba²⁺样品，并对其光谱特性进行 了研究.结果发现，对于由SrO和CeO₂直接反应生成的Sr₂CeO₄(Ⅰ)，激发主峰位于256nm 左右；而对于SrCeO₃和SrO反应生成的Sr₂CeO₄(Ⅱ)，激发主峰位于279nm左右.在Sr₂CeO₄(Ⅰ)中掺入Ca²⁺，其激发光谱随着Ca²⁺离子浓度的增加逐渐接近于Sr₂CeO_{4(Ⅱ)的激发光谱.激发主峰带应属于CeO6八面体终端Ce⁴⁺—O^2-键的电荷迁移 带.对于激发光谱中340nm左右的弱激发峰，其峰值波长不受形成机理及Ca²⁺掺杂的影响，只是其强度 随着 激发主峰的红移而增加，它可能属于CeO6八面体平面上Ce⁴⁺—O2-键的电荷 迁移带.形成机理及Ca²⁺掺杂对发射光谱没有影响.Ca²⁺在Sr 2CeO 4(Ⅱ)与Ba²⁺在Sr2CeO4(Ⅰ)和(Ⅱ)中均难 于替代Sr²⁺的位置.}     

H+Br2→HBr+Br反应的态-态量子动力学研究

H原子与卤素气体(F₂,Cl₂,Br₂)的反应是典型的轻-重-重原子-双原子反应. 对于研究化学激光的基本反应途径十分重要. 之前所有的实验结果都表明,H+Br₂→HBr+Br反应的势垒高度很小,甚至是负值. 本文基于11698个UCCSD(T)/CBS水平的从头算能量点,用FI-NN方法构建了HBr₂体系的精确全维全域势能面,还包括了Br原子²P_3/2轨道的自旋-轨道耦合. 势能面有一个下沉的势垒(-0.351 kcal/mol}),放热(ΔH₀=-41.265 kcal/mol) 和实验值吻合的很好,在这个势能面上应用含时波包方法计算了H+Br₂→HBr+Br反应的态-态积分和微分截面. 对初始基态反应,产物HBr(v′=2,3,4)态在所考虑的整个能量范围内占主导地位,说明HBr是振动态布居反转的. 温度300 K时,计算的产物振动分布在$v$$''$=3有最大值,在v′=0,1的分布可以忽略不计,这与Setser及合作者和Polanyi及合作者的实验结果相一致. 超过一半的总可用能量进入到产物的内部运动中,这其中大部分进入到振动中. 计算表明,反应物Br₂的初始转动激发对产物振转态分布和微分截面影响很小,而初始振动激发则有一定影响. 在低能区域,初始振动激发到v₀=5态很明显的增强了产物的振动激发. 在初始基态和初始转动激发态下,碰撞能量到0.5 eV的微分截面在后向达到峰值,但随着碰撞能量的增加,角分布的宽度显著增加. 对于初始振动激发态,产物微分截面的结构较为复杂,对高振动激发态产物有很强的前向散射峰.     

He-H2S复合物的六维从头算势能面和束缚态

采用[CCSD(T)]-F12a/aug-cc-pVTZ方法，同时在基组中引入中心键函数(3s3p2d1f1g)构建了He-H$_2$S复合物的高精度六维势能面. 除分子间振动坐标，同时考虑了H₂S分子内的v₁对称伸缩振动Q₁正则模、v₂弯曲振动Q₂正则模和v₃反对称伸缩振动Q₃正则模三种振动模式. 将计算得到的六维势能面在Q₁，Q₂和Q₃方向上分别做积分得到H₂S单体分别处于振动基态、v和v₃激发态下的He-H₂S的三个振动平均势能面. 计算结果表明，每个平均势能面都有一个T形全局极小值、一个平面局部极小值、两个平面内鞍点和一个平面外鞍点. 全局极小值的几何构型位于R=3.46 ?，θ=109.9°和φ=0.0°，势阱深度为35.301 ^-1. 在径向部分采用离散变量表象法和角度部分采用有限基组表象法并结合Lanczos循环算法计算了He-H₂S的振转能级和束缚态. 计算发现He-(para-H₂S)在H₂S的v₂和v₃区域的带心位移分别为0.025 cm^-1和0.031 cm^-1，而He-(ortho-H₂S)的带心位移分别为0.041 cm^-1和0.060 cm^-1，都表现为蓝移.     

Br2+分子离子[1+1]双光子解离动力学

本文利用最近研制的低温离子阱-离子速度成像谱仪在冷离子束中研究了同位素质量分辨的⁷⁹Br₂⁺分子离子的[1+1]双光子激光解离动力学. 借助其1⁴Σ^-_u,3/2态为中间态使⁷⁹Br₂⁺共振吸收两个光子至4∽5 eV区域的高激发态并发生解离. 利用离子速度成像技术获得了光解产物⁷⁹Br⁺的二维速度分布和平动能释放谱. 通过平动能释放谱确定了不同解离能量处量子态分辨的解离产物通道分支比. 光碎片产物的角分布表明⁷⁹Br₂⁺分子离子的双光子解离是1⁴Σ^-_u,3/2态的ΔΩ=0平行跃迁至一个Ω=3/2高解离态发生的. 由于分子激发态中的强自旋-轨道耦合作用,高激发的四重态很可能参与到实验观测的光解过程.     

Mg2+掺杂Zn2SiO4:Mn2+的溶胶-凝胶法合成及真空紫外发光特性研究

采用溶胶-凝胶法（sol-gel method）于不同气氛条件下成功合成了Zn_1.92-xMg_xSiO₄:0.08Mn²⁺（0≤x≤0.12）系列粉末样品.利用X射线衍射(XRD)、光致发光(PL)谱等分析手段对Zn_1.92-xMg_xSiO₄:0.08Mn²⁺系列     

新颖的酸催化迈克尔型巯基荧光探针的机理

迈克尔加成反应通常为碱催化的反应,但是在本工作体系当中,2-(2-乙烯基,7-羟基喹啉)丙二酸(QMA)能够被酸催化检测巯基. 从实验和理论计算证明了QMA探测巯基是,且溶液pH值越低,活 性越强. 在碱性溶液中,它的负离子形式QMA[-2H⁺]2^-不能够与电离前或电离后的巯基反应. 与QMA相比,它的酯QME显示出相反的pH效应,这与一般的基于迈克尔加成的巯基荧光探针类似. DFT计算得到的活化焓支持上述两种探针的pH效应. 在酸性溶液中,质子化的QMA与中性和碱性溶液中的负离子形式相比更容易与亲核试剂发生加成,因此能够与低活性的未电离硫醇反应. 相反地,QME与未电离硫醇反应的能垒很高,与电离后的硫醇反应活化能很低. 理论计算研究显示QMA与未电离硫醇的反应为1,4-加成而QME与电离后的硫醇的反应为1,2-加成.     

Dependence of negative ion formation on inhomogeneous electric field strength in atmospheric pressure negative corona discharge

The dependence of negative ion formation on the inhomogeneous electric field strength in atmospheric pressure negative corona discharge with point-to-plane electrodes has been described. The distribution of negative ions HO^-, NO_x ^- and CO_x ^- and their abundances on the plane electrode was obtained with a mass spectrometer. The ion distribution on the plane was divided into two regions, the center region on the needle axis and peripheral region occurring the dominant NO_x ^- and CO_x ^- ions and HO^- ion, respectively. The calculated electric field strength in inhomogeneous electric field established on the needle tip surface suggested that the abundant formation of NO_x ^- and CO_x ^- ions and HO^- ion is attributed to the high field strength at the tip apex region over 10⁸ Vm^-1 and the low field strength at the tip peripheral region of the order of 10⁷ Vm^-1, respectively. The formation of HO^-, NO_x ^- and CO_x ^- has been discussed from the standpoint of negative ion evolution based on the thermochemical reaction and the kinetic energy of electron emitted from the needle tip.     

Single-molecule Detection of Reactive Oxygen Species: Application to Photocatalytic Reactions

In this review, we have focused on the oxidation reactions of single dye molecules by reactive oxygen species (ROS). The methodologies for the single-molecule detection of ROS, such as hydroxyl radical (HO^•), singlet oxygen (O₂(a¹Δ_g)), and hydrogen peroxide (H₂O₂), have been introduced together with examples. In particular, a successful application using the single-molecule fluorescence technique for the investigation of the TiO₂ photocatalytic oxidation reactions is demonstrated in detail.     

Synergistic effect of sonication on photocatalytic oxidation of pharmaceutical drug carbamazepine

Photocatalytic, sono-photocatalytic oxidation of pharmaceutical drug of carbamazepine was successfully carried out using Ag/AgCl supported BiVO₄ catalyst. For this purpose, firstly, photocatalytic oxidation was optimized by central composite design methodology and then synergistic effect of sonication was investigated. Low frequency (20 kHz) probe type and high frequency (850 kHz) plate type sonication at pulse and continuous mode were studied to degrade the carbamazepine (CBZ) containing wastewater. Pulse duties of 1:5 and 5:1 (on : off) were tested using the high frequency sonication system in the sono-photocatalytic oxidation of CBZ. The effects of frequency, power density measured from calorimetry by changing amplitudes were discussed in the sono-photocatalytic oxidation of CBZ. Complete carbamazepine removal was achieved at the optimum conditions of 5 ppm CBZ initial concentration with 1.5 g/L of catalysts loading and at an alkaline pH of 10 at the end of 4 h of photocatalytic reaction under visible LED light irradiation. Both low frequency and high frequency sonication systems caused an increase in photocatalytic efficiency in a shorter treatment time of 60 min. CBZ removal increased from 44% to 65.42% in low frequency sonication of 20 kHz at the amplitude of 20% (0.15 W/mL power density). In the case of high frequency ultrasonic system (850 kHz), CBZ removal increased significantly from 44% to 89.5 % at 75% amplitude (0.12 W/mL power density) within 60 min of reaction. Continuous mode sonication was observed to be more effective than that of pulse mode sonication not only for degradation efficiency and also for electrical energy consumption needed to degrade CBZ. Sono-catalytic oxidation was also conducted with simulated wastewater that contains SO₄^2-, CO₃^2–, NO^3–, Cl^- anions and natural organic component of fulvic acid. The CBZ degradation was inhibited slightly in the presence of NO₃^– and Cl^-, and fulvic acid, however, the existence of SO₄^2- and CO₃^2– increased the degradation degree of CBZ. Toxicity tests were performed to determine the toxicity of untreated CBZ, and treated CBZ by photocatalytic, and sono-photocatalytic oxidations.     

玻碳电极上ABTS的电化学行为

通过循环伏安法和旋转圆盘电极装置研究了2,2′-偶氮-双-(3-乙基苯并噻唑啉-6-磺酸)二铵盐(ABTS),ABTS^2-和ABTS^·-氧化还原对在pH=4.4的磷酸缓冲溶液中和玻碳电极上的电化学和传质行为. 由不同转速下记录的i-E曲线, 得到在磷酸缓冲溶液的电极反应速率常数和传递系数以及ABTS^2-的扩散系数分别为4.6×10^-3 cm/s、0.28和4.4×10^-6 cm^{2相似文献}   

Kinetic modeling of the benzyl + HO2 reaction

Benzyl is a resonantly stabilized radical that commonly occurs as an intermediate in the combustion of aromatic compounds. The bimolecular reaction of benzyl with HO₂ is important in the oxidation of toluene, especially at low to moderate temperatures, where unimolecular decomposition of the benzyl radical is slow. We show that the addition of HO₂ to the methylene site in benzyl produces a vibrationally excited benzylhydroperoxide adduct, with over 60 kcal mol⁻¹ (251 kJ mol⁻¹) of excess energy above the ground state. RRKM simulations are performed on the benzyl + HO₂ reaction, using thermochemical and kinetic parameters obtained from ab initio calculations, with variational transition state theory (VTST) for treatment of barrierless radical + radical reaction kinetics. Our results reveal that the benzyl + HO₂ reaction proceeds predominantly to the benzoxyl radical + OH at temperatures of around 800 K and above, with the production of stabilized benzylhydroperoxide molecules dominating at lower temperatures. The heat of formation of the benzyl radical is calculated as 52.5 kcal mol⁻¹ (219.7 kJ mol⁻¹) at the G3B3 level of theory, in relative agreement with other recent determinations of this value.     

Vibrational non-equilibrium in the hydrogen–oxygen reaction. Comparison with experiment

A theoretical model is proposed for the chemical and vibrational kinetics of hydrogen oxidation based on consistent accounting of the vibrational non-equilibrium of the HO₂ radical that forms as a result of the bimolecular recombination H+O₂ → HO₂. In the proposed model, the chain branching H+O₂ = O+OH and inhibiting H+O₂+M = HO₂+M formal reactions are treated (in the terms of elementary processes) as a single multi-channel process of forming, intramolecular energy redistribution between modes, relaxation, and unimolecular decay of the comparatively long-lived vibrationally excited HO₂ radical, which is able to react and exchange energy with the other components of the mixture. The model takes into account the vibrational non-equilibrium of the starting (primary) H₂ and O₂ molecules, as well as the most important molecular intermediates HO₂, OH, O₂(¹Δ), and the main reaction product H₂O. It is shown that the hydrogen–oxygen reaction proceeds in the absence of vibrational equilibrium, and the vibrationally excited HO₂(v) radical acts as a key intermediate in a fundamentally important chain branching process and in the generation of electronically excited species O₂(¹Δ), O(¹D), and OH(²Σ⁺). The calculated results are compared with the shock tube experimental data for strongly diluted H₂–O₂ mixtures at 1000 < T < 2500 K, 0.5 < p < 4 atm. It is demonstrated that this approach is promising from the standpoint of reconciling the predictions of the theoretical model with experimental data obtained by different authors for various compositions and conditions using different methods. For T < 1500 K, the nature of the hydrogen–oxygen reaction is especially non-equilibrium, and the vibrational non-equilibrium of the HO₂ radical is the essence of this process. The quantitative estimation of the vibrational relaxation characteristic time of the HO₂ radical in its collisions with H₂ molecules has been obtained as a result of the comparison of different experimental data on induction time measurements with the relevant calculations.     

Negative ion formation and evolution in atmospheric pressure corona discharges between point-to-plane electrodes with arbitrary needle angle

The change in the distribution pattern of negative ions HO^–, NO_x^-_{x}^{-} and CO_x^-_{x}^{-} observed on arbitrary point-to-plane electrode configuration has been investigated by varying the angle of needle to the plane electrode, under atmospheric pressure corona discharge conditions. The stationary inhomogeneous electric field distributions between the point-to-plane electrodes with arbitrary needle angle were calculated. The experimental and theoretical results obtained suggested that the negative ion evolutions progress along field lines established between the electrodes with arbitrary configurations and the resulting terminal ion formation on a given field line is attributable to the electric field strength on the needle tip surface where the field line arose. The NO_x^-_{x}^{-} and CO_x^-_{x}^{-} ions were dominantly produced on the field lines arising from the needle tip apex region with the highest electric field strength, while the field lines emanating from the tip peripheral regions with lower field strength resulted in the formation of the HO^– ion.     

光电子成像研究AgOCH3-和Ag-(CH3OH)x (x=1, 2)

用光电子成像技术和从头算法研究Ag^-(CH₃OH)_x (x=1, 2)和AgOCH₃^-. 从AgOCH₃^-振动分辨的光电子谱得 到AgOCH₃^-的绝热和垂直电离能分别为1.29(2)和1.34(2) eV. Ag^-(CH₃OH)_{1,2相似文献}   

Effect of a single water molecule on the formations of H2O2 + ClO from HO2 + HOCl reaction under tropospheric conditions

ABSTRACT

In this work, four different channels, represented by H₂O???HO₂ + HOCl, HO₂???H₂O + HOCl, H₂O???HOCl + HO₂ and HOCl???H₂O + HO₂ have been analysed for water-catalysed formations of H₂O₂ + ClO to gain insight into the potential impact of the reaction in the atmosphere. The results at the CCSD(T)/aug-cc-pVTZ//MP2/6-311+G(2df,2p) level show that the H₂O???HO₂ + HOCl reaction is kinetically the most favourable channel among the four channels. Compared to the channel of H₂O₂ + ClO formations without water vapour, the effective rate constant of H₂O???HO₂ + HOCl reaction is estimated to be faster than the naked reaction by 2–3 orders of magnitude, indicating that the single water molecule in the H₂O???HO₂ + HOCl channel exhibits a positive catalytic effect on enhancing the rate of H₂O₂ + ClO formations. Meanwhile, it is interesting that the transfer process between H₂O???HOCl + HO₂ and H₂O???HO₂ + HOCl has an activation energy of 0.6 kcal?mol^?1 and can occur easily under tropospheric conditions.