Flow injection analysis methods for determination of diffusion coefficients

Two flow injection analyses (FIA) methods for the determination of diffusion coefficients in a straight single tube FIA system were developed. Based on the analytical solution of the convection-diffusion equation, linear relationships of the logarithmic values of the dispersion coefficient (D) and the half-peak width (W_1/2) with the diffusion coefficient (D_m) were obtained. Experiments were designed to verify these methods. For example, for potassium hexacyanoferrate (III) a D_m value of 0.72 × 10⁵ cm² s⁻¹ was found versus a literature value of 0.76 × 10⁵ cm² s⁻¹ (error, 5%). For potassium hexacyanoferrate (II) a D_m value of 0.67 × 10⁵ cm² s⁻¹ was obtained versus a literature value of 0.63 × 10⁵ cm² s⁻¹ (error, 6%). The diffusion coefficients of some important biomedical compounds, such as dopamine, epinephrine, norepinephrine and ascorbic acid, were then determined. The values of 10⁵ D_m/cm² s⁻¹ are 0.60 ± 0.03, 0.44 ± 0.02, 0.60 ± 0.01 and 0.68 ± 0.06, respectively.     

Update of the anharmonic force field parameters of the ozone molecule

A new set of spectroscopic constants of the ¹⁶O₃ molecule (ω_i, x_ij, y_ijk, γ^DD, _i^X, β_ij^X,…), which determine vibrational dependence of band centres and rotational parameters, is derived from recent accurate analysis of high-resolution experimental ro-vibrational spectra through the theoretical approach based on second-order perturbation expansions in normal coordinates accounting for Darling–Dennison resonance interactions. These values are used to update empirical values of anharmonic coefficients (k_ijl, k_ijlm) of the potential function expansion in normal coordinates. Quadratic f_rr, f_r, f_rr′, f as well as cubic f_rst and quartic f_rstl force constants in internal (bond lengths, bond angle) coordinates are also derived. A detailed discussion is devoted to the accuracy of parameter determination for each of four steps of calculations. It is emphasised that the conventional method based on the inversion of formulae of the perturbation theory gives the largest uncertainties at the last step of calculations: the determination of the anharmonic force field in internal coordinates.     

2-甲基呋喃分子激发态超快非绝热动力学

Excited-state dynamics of 2-methyl furan has been studied by femtosecond time-resolved photoelectron imaging. The molecule 2-methyl furan was simultaneously excited to the n=3 Rydberg series of S₁[¹A"(π3s)], ¹A'(π3p_x), ¹A"(π3p_y) and ¹A"(π3p_z) and the valence state of ¹A'(ππ^*) by two 400 nm photons and subsequently probed by two 800 nm photons. The average lifetime of the Rydberg series and the valence state was measured to be on the time scale of 50 fs by the time-dependent ion yield of the parent ion. Ultrafast internal conversions among these excited states were observed and extracted from the time-dependences of the photoelectron kinetic energy components of these excited states in the photoelectron kinetic energy spectra. Furthermore, it is identified that the ¹A'(ππ^*) state might play an important role in internal conversions among these excited states. The Rydberg-valence mixings, which result in numerous conical intersections, act as the driving force to accomplish such ultrafast internal conversions.     

Oxygen potential and phase equilibria in the Te-Sb2O3-Sb2O4 pseudoternary part of the Sb-Te-O system at elevated temperatures

Employing the electrochemical cells with the solid oxide electrolyte

Kanthal + Re, Te(l), TeO₂(s)O⁻² air, Pt

Pt + Re, Sb₂O₃(s), Sb₂O₄(s)O⁻² air, Pt

Pt + Re, Sb₂O₃(s), Sb₂O₄(s), Te(l)O⁻² air, Pt

the equilibrium oxygen potential in the pseudobinary Te-TeO₂, Sb₂O₃-Sb₂O₄ and in the Sb₂O₃-Sb₂O₄-Te pseudoternary systems was determined in the temperature range 700-1173 K. In addition, the pseudobinary sections Sb₂O₃-Te, Sb₂O₃-Sb₂O₄ (1:1)-Te and Sb₂O₄-Te were examined by DTA in the temperature range 500-1300 K. Using these results the evolution of the pseudoternary system with temperature can be suggested. It was found that, at 718 K, a ternary eutectic with a composition close to pure Te appears in the system. At a higher temperature, 920 K, another liquid phase is formed, which is characteristic of the ternary four-phase equilibrium L₂ + Sb₂O₄(s) + Sb₂O₃(s) = L₁.     

The fabrication and performance of an Ag/AgCl reference electrode in human serum

A simple set of electric circuits was used to assemble a pulse generator. With pulse potentials and under galvanostatical control, a clean silver wire was anodized electrochemically for 0.2–0.5 min in 1.0 mol l⁻¹ HCl with a pulse current density of 20 mA cm⁻², and the pulse wave parameters of t_a/t_c = 1 and a cycle of 4 s forming an Ag/AgCl reference electrode. Even though the AgCl layer was consumed during the working period when the Ag/AgCl electrode was used as a cathode, the AgCl layer could be in situ recovered electrochemically in serum used when a reversed potential was applied to the electrode system immediately after the measuring program was finished. The current response curve of the anode indicated that an AgCl layer in high density was basically accomplished during the first 6 pulse cycles in human serum. In order to keep a stable and uniform AgCl layer on the reference electrode after each measuring cycle, the ratio of the recovery time (t_r) to the working time (t_w) was measured and the smallest value was obtained at 0.03. The open-circuit potential of the Ag/AgCl electrode with respect to a SCE in 0.1 mol l⁻¹ KCl was monitored over a period of 14 days and the mean value was 40.09 mV vs SCE with a standard deviation of 2.55 mV. The potential of the Ag/AgCl reference electrode did remain constant when the measurements were repeated more than 600 times in undiluted human serum with a standard deviation of 1.89 mV. This study indicated that the Ag/AgCl reference electrode could been rapidly fabricated with a pulse potential and could be used as a reference electrode with long-term stable properties in human serum samples.     

Accurate base composition of double-strand DNA by mass spectrometry

An accurate molecular weight (M_r) assignment for a double-strand (ds) DNA determines or greatly restricts the possible number of each of its four bases, while the compositions for its two single-strand (ss) components can also be derived from their M_r values. For a ds 64-mer (39 kDa), the ss-M_r values (± 0.5 Da) of its high-resolution mass spectrum from an electrospray ionization/Fourier transform instrument yield only the correct ds- and ss-base compositions. Literature mass spectra of lower mass accuracy show that such data can also restrict their possible composition assignments, with further discrimination using the abundance vs. base composition of small fragment ions from the dissociation of the ss molecular ions.     

第一性原理研究混合钙钛矿CH3NH3PbxSn1－xI3结构及光电特性

有机/无机钙钛矿是一类极具潜质的光电材料,目前已实现超过20%的光电转化效率。本文采用第一性原理对有机/无机混合钙钛矿CH₃NH₃Pb_xSn_1-xI₃ (x = 0-1)的结构及光电特性进行了理论研究。结果表明,范德华力(VDW)在优化钙钛矿结构中起着重要的作用,考虑范德华力可减小Pb/Sn―I键长,从而减小体系体积。通过分析甲胺离子CH₃NH₃⁺的态密度和Bader电荷,我们发现其对前线轨道没有贡献,仅仅扮演电荷供体的角色。Pb/Sn与I之间同时存在共价键和离子键相互作用。价带顶(VBM)主要是由I 5p以及Pb 6s (Sn 5s)杂化组成,而导带底(CBM)主要由Pb 6p (Sn 5p)轨道组成。在可见光区,随着波长的增加,体系吸收强度呈现整体下降趋势;随着Sn/Pb比值逐渐增大,吸收强度呈现增大趋势。CH₃NH₃SnI₃在可见光区表现出较佳的吸收光谱特性。     

Photodecomposition of molybdenum(II) and tungsten(II) carbonyl complexes with triazole, benz-imidazole, and oxadiazole acetylinic derivatives

Photodecomposition of 10 different molybdenum and tungsten mixed carbonyl complexes, [M(CO)₃(B)(A)]I₂ where B=o-phenanthroline or bipyridyl, A=3-(2-propynyl)thio-4,5-diphenyl-4H-1,2,4-triazole (TRZA) or S-propynyl-2-thio benz-imidazole (BIMDA) and 2(2-propynyl-thio(5-phenyl)-1,3,4-oxadiazole (OXA). M(CO)₃(TRZA)I₂, [M(CO)₂(PPh₃)_X(TRZA)I_Y]I_Z where M=Mo, X, Y and Z=1 and M=W, X and Z=2, Y=0, have been performed at 365 nm in oxygen saturated chloroform at 25 °C. The absorbance spectrum of these complexes have been recorded with the time of irradiation in order to examine the kinetics of photodecay.

The apparent rate constant (K_d) for the first-order reaction have been calculated and found to be (3.32–4.79)×10⁻⁵ s⁻¹. The primary quantum yields (Φ) has also been calculated and were in the range (8.33–12.1)×10⁻⁴. The mechanism of the photodecomposition has been suggested according to the kinetic, and photoproduct analysis data, and is similar to reaction of photo-oxidative degradation of polluted molecules in the water.     

Evaluation of carrier gases for use in high-field asymmetric waveform ion mobility spectrometry

Effects of carrier gas type (N₂, O₂, CO₂, N₂O, and SF₆) on changes in the ratio of high- to low-field ion mobility, K_h/K, of cesium, gramicidin S, tetrahexylammonium, heptadecanoic acid, and aspartic acid in fields of up to 67 Td are presented. The theory of the mobility of ions at high E/N in different gases is discussed. Plots of K_h/K as a function of the ionic energy parameter, E/N, for the five ions in each of the gases were derived from experimental data collected using a high-field asymmetric waveform ion mobility spectrometer. The change in the ratio of high- to low-field ion mobility of cesium in carrier gases of O₂ and N₂ showed excellent agreement with literature values. The behavior of cesium in O₂ and N₂ is used to illustrate that the ratio K_h/K as a function of effective temperature is invariant with gas type as long as the well depth of the interaction potential significantly exceeds thermal energy. From these results, it appears that the well depth of the interaction potential of the heavier ions studied here, including gramicidin S, tetrahexylammonium, and heptadecanoic acid, with bath gases such as N₂ and O₂, is shallow relative to thermal energy.     

Equilibrium of the reaction between dissolved sodium sulfide and biologically produced sulfur

The equilibrium of the heterogeneous reaction between dissolved sodium sulfide and biologically produced sulfur particles has been studied. Biologically produced sulfur was obtained from a bioreactor of a hydrogen sulfide removal process in which the dominating organism is Thiobacillus sp. W5. Detailed knowledge of this reaction is essential to understand its effect on the process. The results were compared with the equilibrium of the reaction of sulfide with ‘inorganic’ elemental sulfur. The equilibrium between dissolved sodium sulfide and biologically produced sulfur particles can be described by an equilibrium constant, K_x, which consists of a weighted sum of constants for polysulfide ions of different chain length, rather than a true single equilibrium constant. For biologically produced sulfur pK_x = 9.10 ± 0.08 (21 °C) and 9.17 ± 0.09 (35 °C) with an average polysulfide chain length x = 4.91 ± 0.32 (21 °C) and 4.59 ± 0.31 (35 °C). The pK_x value for biologically produced sulfur is significantly higher than for reaction of dissolved sodium sulfide with inorganic sulfur (pK_x = 8.82; 21 °C). This difference is probably caused by the negatively charged polymeric organic layer, which is present on biologically produced sulfur but absent with “inorganic” sulfur. Specific binding of polysulfide ions to the organic layer results in a higher polysulfide concentration at the reaction site compared to the bulk concentration. This results in an apparent decrease of the measured equilibrium constant, K_x.     

Chalcogenide based all-solid-state thin electroplated ion-selective membrane for Hg(II) flow-injection determinations

The response to Hg(II) of a thin all-solid-state Te-doped silver chalcogenide membrane, described by the general formula Ag₂ + δSe_{1 − x}Te_x, which has been electrochemically prepared following a previously proposed approach, has been investigated. The kinetics of formation of the membrane's secondary dynamic response to Hg(II) has been successfully combined with the precise timing and transient signal, typical for flow-injection (FI) measurements, in developing a sensitive and reliable mercury FI detector. Under optimized stream conditions it exhibits a linear Nernstian response, with a double slope of the calibration graph of 59 mV dec⁻¹, over the mercury(II) concentration range 10⁻⁶ − 10⁻³ M, the typical sample throughput amounting to about 70 samples per hour. The observed chemical amplification of the signal is due to the specificity of the processes dominating the initial step in formation of the steady-state signal of the membrane to mercury. The analytical performance of the Hg(II) FI detector, as regards sensitivity, reproducibility, selectivity and long-term stability has been thoroughly investigated. The exact procedure for membrane electrodeposition is given and the potential of the proposed approach as a cost-effective way for preparing chalcogenides of unique structure and properties has been outlined in the above context.     

Preparation of dense, ultra-thin MIEC ceramic membranes by atmospheric spray-pyrolysis technique

Dense ceramic mixed ionic and electronic conducting membranes have been deposited by atmospheric spray-pyrolysis technique onto porous ceramic substrates. Perovskite oxide layers, i.e. manganites La_1−xSr_xMnO₃, ferrites La_1−xSr_xFe_1−y(Co,Ni)_yO₃, gallates La_1−xSr_xGa_1−y(Co,Ni,Fe)_yO₃, cobaltites La_1−xSr_xCoO₃ and related perovskites such as lanthanum nickelate La₂NiO₄ layers have been prepared. The structure, morphology and composition of the layers were characterised by XRD, SEM and WDS, respectively. Density and gas tightness of the layers were studied as a function of deposition process parameters, film thickness (from 0.5 to 3 μm) and preparation procedure. The presence of cracks and defects due to thermo-mechanical stresses applied during or after the preparation process were correlated with the membrane composition and the corresponding thermal expansion coefficient differences between substrates and membranes.     

Millimeter-wave rotational spectrum and molecular constants of diatomic gallium iodide

The gas-phase molecular spectrum of Gal has been detected in the millimeter wavelength region. The molecules are produced by vapourising a mixture of gallium and lead iodide into an evaculated cell. Analysis of the observed rotational transitions yields the following molecular parameters for ⁶⁹Ga¹²⁷I: Y₀₁ = 1706.89645(83) MHz, Y₁₁ = −5.68714(53) MHz, Y₂₁ = 6.329(43) kHz, Y₀₂ = −0.472713(60) kHz, Y₁₂ = 0.472(38) Hz, ω_e = 216.38 cm⁻¹, ω_e^x_e= 0.471 cm⁻¹, and for ⁷¹Ga¹²⁷I: y₀₁ = 1675.72004(71) MHz, Y₁₁ = −5.53277(57) MHz, Y₂₁ = 5.995(34) kHz, Y₀₂ = −0.455700(51) kHz, y₁₂ = 0.522(40) Hz, ω_e = 214.37 cm⁻¹, and ω_e^x_e = 0.458 cm⁻¹. The equilibrium internuclear distance obtained for Gal is r_e = 2.574667(12) Å.     

Inverse deuterium isotope effect on radiationless electronic transitions

Fluorescence quantum yields, Y, front photoselected vibrational states in the S₁ manifold of anthracene and of perdeuterated anthracene in planar supersonic jets reveal a large inverse deuterium isotope effect on the non-radiative relaxation from the S₁ origin (Y_H/Y_D = 5), while for high (1500 cm⁻¹) excess energies above the S₁ origin the inverse isotope effect is eroded (Y_H/Y_D ≈ 1). Novel information emerges on intermediating states involved in intersystem crossing.     

The interaction between C28 (Td) and X (X=H and F)

Hydrogen and fluorine addition reactions with C₂₈(T_d) have been investigated by the density function theory method at B3LYP/6-31G level. The interaction potential between C₂₈(T_d) and atom X (X=H and F) shows that there are three possible stable isomers of C₂₈(T_d)X (X=H and F) and the average binding energy calculations suggest that C₂₈(T_d)H₄ is the most stable hydrogen adduct among C₂₈(T_d)H_n (n=1–28). Furthermore, by comparisons of the energy between C₂₈(T_d)H and C₂₈(C_s)H we found that the former are more stable than the later, and the structural and energy analysis further indicate that C₂₈(C_s)H is only with a small distortion of C₂₈(T_d)H symmetry. In addition, the transition states, as well as reaction pathways of X transfer reactions between different key points on C₂₈(T_d) representative patch are given to explore the possible reaction mechanism.     

综合利用稻壳制备木糖、电容炭与硅酸钙晶须

利用酸水解稻壳中的半纤维素制备木糖, 并将糖渣经过炭化后分离出碳和硅, 碳采用稀碱溶液活化改性制备电容炭, 硅采用水热法合成了硅酸钙晶须, 从而使稻壳所有组分得到充分利用. 采用循环伏安(CV)和恒流充放电(GCD)研究了电容炭的电化学性能. 通过X射线衍射(XRD)和扫描电子显微镜(SEM)对所得硅酸钙晶须的结构和形貌进行了表征. 实验结果表明, 稻壳酸水解的最优条件为硫酸浓度7%(质量分数)、 固液比(g/mL)为1:8、 反应时间为2.0 h, 在该条件下, 一次水解、 二次水解和三次水解的木糖收率(Y₁/Y₂/Y₃)和浓度(质量分数, C₁/C₂/C₃)都能达到最大值, Y₁=98.5%, C₁=3.6%; Y₂=85.4%, C₂=6.3%; Y₃=76.6%, C₃=9.0%. 采用15 mL 8%(质量分数) NaOH稀碱溶液活化改性制得的电容炭(AC/15)比电容值为77.32 F/g, 而且具有较好的倍率性和循环稳定性; 硅酸钙晶须为扫帚状针钠钙石晶须.     

Upper and lower critical solution temperatures in polybutadiene-alkane systems : Effect of the surface-to-volume ratio of the polymer

Cloud point curves (CPC) have been measured for 1–4 cis polybutadiene (M_r = 40,000–830,000) in n-hexane, 2-methyl-hexane, 2,2,3 trimethylbutane and 2,2,4 trimethylpentane. These four systems show upper and lower critical solubility temperatures which approach one another as the molecular weight increases. An hourglass-shaped CPC is found for two systems. The CPC are found to be much more dependent on polymer concentration than is usual. Calculated (Prigogine, Patterson, Flory theories) and experimental critical temperatures, critical volumes and shapes of the CPC are in much better agreement for these systems than for other systems involving polystyrene, polyisobutylene or polybutene-1. Analysis of these results with those for other systems in the literature indicates the importance of the surface-to-volume ratio s of the polymers. A small value of s = s₂/s₁ (0·5–0·8) for thick polymer chains improves the calculated value of the critical temperature while s = 1 is quite good for thin polymer chains such as polybutadiene and polyethylene.     

The molecular structure of beryllocene, (C5H5)2Be. A reinvestigation by gas phase electron diffraction

The electron scattering pattern of gaseous dicyclopentadienylberyllium, Cp₂Be, has been recorded from s = 2.00 to 39.00 Å⁻¹ with a nozzle temperature of about 120°C. Molecular models of D_5d symmetry or models containing one π-bonded and one σ-bonded Cp ring are not compatible with the data. The possibility the gaseous Cp₂Be consists fo a mixture D_5d and π-Cp, σ-Cp conformers is considered and rejected. A model of C_5v symmetry can be brought into satisfactory agreement with the data. It is also found that a slip sandwich model obtained from the C_5v model by moving sideways the ring which is at the greatest distance from Be, while keeping the two rings essentially parallel is compatible with the electron diffraction data. The best fit between experimental and calculated intensity curves is obtained with a model with a sideways slip of 0.8(1) Å. This model is similar to that indicated by the X-ray diffraction investigations by Wong and coworkers [4,5]. It is suggested that the potential energy of the molecule does not change much as the magnitude of the slip changes and that the molecule thus undergoes large amplitude vibration.     

TiN/HfxZr1-xO2/TiN铁电电容器的原位生长与表征

HfO₂基铁电电容器,特别是TiN/Hf_xZr_1-xO₂/TiN金属-绝缘体-金属电容器,由于其良好的稳定性、高性能和互补金属氧化物半导体(CMOS)兼容性,在新一代非易失性存储器中有着广阔的应用前景。由于TiN/Hf_xZr_1-xO₂/TiN电容器的电性能与Hf_xZr_1-xO₂铁电薄膜与TiN电极层界面质量相关,因此控制TiN/Hf_xZr_1-xO₂/TiN异质结构的制备和表征至关重要。本文报道了一种三明治结构：Hf_xZr_1-xO₂铁电薄膜夹在两个TiN电极之间的新的制备方法,通过超高真空系统互连的原子层沉积(ALD)和磁控溅射设备实现。原位生长和表征结果表明,ZrO₂掺杂浓度和快速热退火温度可以调节TiN/Hf_xZr_1-xO₂/TiN异质结的铁电性能,并能很好地被互连系统监控。在该体系中,通过在HfO₂中掺杂50% (molar fraction, x) ZrO₂并且在600 ℃下快速热退火(RTA),获得了21.5 μC·cm^-2的高剩余极化率和1.35 V的低矫顽电压。     

Many-body effects in polymers: especially polyacetylene

Many-electron effects in polymers are considered, with emphasis on the way electron-electron interactions are reflected in ground-state properties. After a survey of results on graph theory, built up from valence-bond structures, in which the importance of size consistency again emerges, some specific results of ground-state electron pair correlations in polyacetylene and polydiacetylene are considered, motivated by the linear dispersion of the π-electron plasmon, as measured in the optical experiments of Ritsko et al. The way in which such collective excitations can affect ground-state pair correlations is discussed as is the influence of low dimensionality. A brief summary is given of the way in which the energy gap in polyacetylene and polydiacetylene depends on electron-electron repulsion although unlike the plasmon problem where the long-range Coulomb repulsion e²/r_ij is essential, this problem is usefully tackled using the on-site Hubbard repulsion. Again, there can be no doubt that correlation is important in the ground states of polyacetylene and polydiacetylene. However, recent work on bond-charge repulsion shows that whether correlation enhances or suppresses dimerization depends strongly on the particular thermodynamic state in question: this is illustrated by specific examples relating to the metal-insulator transition in low-dimensional solids. A quite different aspect of many-body phenomena will then be considered, pertaining especially to AC electrical transport in biopolymers. Here, the importance of disorder in the experimental results currently available is stressed. A power law behaviour of the frequency-dependent conductivity, i.e. σ(ω) proportional to ω^s, is a characteristic feature at suitably high frequencies. This focusses attention on the power, s, and a brief discussion of simple models shows that, for those considered to date s< 1, with possible values of 1/4 and 1/2 being exhibited. A possible influence of a compensation effect on the high-frequency conductivity is suggested. It is argued, following Kreuzer and March, that this is a many-particle phenomenon ANDS = 1-(T/T_c) for T < T_c, where T_c is the compensation temperature; a result apparently due to Dyre. The possibility of further experimental and theoretical studies related to the many-body phenomena is referred to.