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1.
Natural salt minerals often contain inclusions of saturated salt solutions with diameters from 1 to> 100 μm. With the quantification of the composition of the fluid inclusions, the origin and metamorphism of the salt rocks can be interpreted. Hence, these data are important concerning the long-term safety of underground repositories in salt rocks [1]. For the extraction of the solutions in fluid inclusions with diameters 300 μm, an optical precision instrument was developed. For the simultaneous determination of Cl, Br, SO42−, Li+, Na+, K+, Mg2+ and Ca2+ two ion chromatographic systems with conductivity detection for cations and anions and additional photometric detection for Br were used. To prevent column overload, the Cl concentration must be less than 50 μg/ml in the measuring solution. The extracted samples (volumes> 0.1 μl) are diluted with demineralized water by a factor of 1 · 104 (20-μl sample loops). The practical limit of determination for the measured elements is 0.01–0.3 μg/ml in the measuring solutions. By calculation of the anion and cation charge balance (molar equivalence), a relative error of <5% for the analysis of fluid inclusions was found.  相似文献   

2.
Analysis of changes in 35Cl NQR frequency of complexes MCl4.L and MCl4.2L for M = Si, Ge, Sn and Ti was performed. The population of the atomic orbitals was calculated by the quantum chemistry methods PM3 and INDO. The results provided an explanation of the changes in 35Cl NQR frequency and the asymmetry parameter upon complex formation. In the complexes of non-transition elements, a decrease in 35Cl NQR frequency is first of all related to increasing population of pz orbitals on Cl atoms. In the complexes of Ti, the increase in 35Cl NQR frequency depends on a decrease in the pπ to dπ electron density transfer.  相似文献   

3.
Analysis of changes in 35Cl NQR frequency of complexes MCl4.L and MCl4.2L for M = Si, Ge, Sn and Ti was performed. The population of the atomic orbitals was calculated by the quantum chemistry methods PM3 and INDO. The results provided an explanation of the changes in 35Cl NQR frequency and the asymmetry parameter upon complex formation. In the complexes of non-transition elements, a decrease in 35C1 NQR frequency is first of all related to increasing population of pz orbitals on Cl atoms. In the complexes of Ti, the increase in 35Cl NQR frequency depends on a decrease in the pπ to dπ electron density transfer.  相似文献   

4.
Fractions of Cu and Zn species in legume samples (common white bean, pea, chick pea and lentil seeds and defatted soybean flour) were analysed by on-line hyphenation of size exclusion chromatography and inductively coupled plasma-mass spectrometry. Samples were extracted by 0.02 mol l−1 Tris–HCl buffer solution, pH 7.5. The extraction efficiency lay in the region 60–90 and 60–80% for Cu and Zn, respectively. Quantification of elements in the individual chromatographic fractions was carried out by isotope dilution (ID) and external calibration (EC) techniques. For ID analysis the chromatographic effluent was mixed with the flow of 65Cu and 68Zn isotope enriched solution and the isotope ratio values 63Cu/65Cu and (64Zn+66Zn)/68Zn were measured. In the case of EC technique calibration solutions of elements were injected to the flow of mobile phase by the second injector. Prior entering detector the effluent was mixed with the flow of internal standard solution (In, 50 μg l−1). Both methods have similar precision, however the behaviour of both studied elements was not the same. The chromatographic analysis itself was the main source of variability in the case of Cu. For Zn species analysis, the extraction process and the manipulation with the extract, played the significant role too. It was probably caused by lower stability of the present zinc chelates. The total amounts of Zn found in all chromatographic fractions represented 85–95% of Zn in sampled extract whereas those of Cu approached 100%. In case of small peaks the results of ID and EC were not the same. The EC results were lower then ID results. The great deal of results uncertainty accounts for the precision.  相似文献   

5.
Hydrogenchalcogenido complexes of general composition (η5-C5R5)(CO)3M(EH) (R = H, CH3; M = Cr, Mo, W; E = S, Se) can be obtained by three different routes, sometimes in quite good yields. Thus, the sulfur and selenium derivatives can be synthesized by insertion of the respective elements into the metal-hydrogen bonds of the precursor compounds (η5-C5R5)(CO)3MH. This species also reacts with potassium selenocyanate to yield the hydrogenselenido derivatives (η5-C5R5)(CO)3M(SeH) which can also be obtained by treatment of the methyl complexes (η5-C5R5)(CO)3M(CH3 (M = Mo, W) with HBF4 and Li[SeH]. The corresponding hydrogentellurido compounds are probably formed by these preparative methods but appear to be quickly converted into either the dinuclear tellurium bridge products (μ-Te)[(η5-C5R5)(CO)3M]2 (M = Mo) or into the hydrido complexes (η5-C5R5)(CO)3MH (M= Mo, W) by release of elemental tellurium.  相似文献   

6.
A laser ablation system using a Nd:YAG laser was coupled both to a quadrupole inductively coupled plasma (ICP) mass spectrometer and to a double-focusing sector field ICP mass spectrometer. Laser ablation inductively coupled plasma mass spectrometry (LA-ICP-MS) was applied for the determination of long-lived radionuclides in a concrete matrix. The investigated samples were two laboratory standards with a concrete matrix, which we doped with different long-lived radionuclides (e.g. 99Tc, 232Th, 233U, 237Np) from the ng g−1 to μ g−1 concentration range and an undoped concrete material (blank). Detection limits for long-lived radionuclides in the 10 ng g−1 range are reached for LA-ICP-MS using the quadrupole mass spectrometer. With double-focusing sector field ICP-MS, the limits of detection are in general one order of magnitude lower and reach the sub ng g−1 range for 233U and 237Np. A comparison of mass spectrometric results with those of neutron activation analysis on undoped concrete sample indicates that a semiquantitative determination of the concentrations of the minor and trace elements in the concrete matrix is possible with LA-ICP-MS without using a standard reference material.  相似文献   

7.
In this paper some synthetic procedures to obtain (η6-arene)metal derivatives are reviewed. The metal-atom-arene-vapor co-condensation technique is the most appropriate to generate complexes of polycyclic aromatic hydrocarbons or heterocycles. As far as the aluminium halide-mediated synthesis is concerned, two classes of reaction are observed. When AlX3 is used with a metal halide in the presence of an aromatic hydrocarbon in the absence of any reducing agent, AlX3 can function as a dehalogenating agent, to give ionic compounds of general formula [M(η6-arene)n](AlX4)m, or it can add across the M---X bond with formation of M(μ-X)nAlX4−n systems. In both cases the metal displays its typical oxidation state. However, the use of AlX3 in combination with aluminium (the Fischer-Hafner reducing system) affords ionic or covalent low-oxidation-state metal(η6-arene) complexes. Attention is focused on our most recent results concerning the synthesis, properties and reactivity of η6-arene derivatives of Group 4 and 5 elements, showing, inter alia, the first example of a tetraarylborate anion behaving as a 12-electron donor to one metal atom and low-valent η6-arene compounds as useful reagents in the inorganic and coordination chemistry of the corresponding metal in nonaqueous systems.  相似文献   

8.
The electronic dipole transition moment functions of the A 2Π-X 2Σ+, B 2Σ+-X 2Σ+ and B 2Σ+-A 2Π transitions and the dipole moment function of the X 2Σ+ state of CO+ have been calculated using large contracted CI wavefunctions. The computed transition moment functions together with experimental potential energy curves were used to obtain radiative lifetimes of the excited electronic states B 2Σ+ and A 2Π. Radiative lifetimes of vibrational levels of the X 2Σ+ state were derived from the calculated dipole moment function. The high-frequency deflection technique was used to obtain radiative lifetimes of the ν′ = 0, 1,2 and 3 vibrational levels of the B 2Σ+ state and also radiative lifetimes of individual rotational levels of ν′ =0. The calculated radiative lifetimes are shorter than the measured ones by about 10%. The experimental ν′ dependence is reproduced by theoretical calculation. The calculated radiative lifetimes for the A 2Π state are in excellent agreement with lifetimes measured with an ion trap technique.  相似文献   

9.
The Ca(1D2, 3PJ) + CH3 → CaI(A,B) + CH3 reactions system has been studied by measuring its chemiluminescence under beam-gas conditions. Absolute values of the state-to-state reaction cross-sections were determined at low collision energy . In addition, the electronic branching ratio and product energy disposal have been determined for each metastable reaction. The major changed observed in the chemiluminescence when comparing the Ca(1D2) reaction versus that of Ca(3PJ) is the total yield associated with the former reaction. To the best of our spectral resolution neither the electronic branching ratio e.g. CaI(A)/CaI(B) nor the internal CaI energy disposal change significantly as the metastable Ca(1D2)/Ca(3PJ) ratio is varied. In spite of the fact that the Ca(3PJ) reaction is less exoergic, the CaI product appears with a higher fraction of internal energy than that of Ca(1D2) reaction. Thus, the fraction of the total energy appearing in CaI internal energy amounts to 57.5% in the Ca(3PJ) reaction while it is 19.3% only for the Ca(1D2) reaction. This difference is discussed in the light of a distinct mechanism associated with the attack of the excited Ca atom into the C---I bond. No significant chemiluminescence yield was found for the energetically open CaCH*3 channels.

The product chemiluminescence polarization was also measured as a function of the metastable concentration. A significant degree of polarization was found depending upon the specific electronic excitation. The analysis of the polarization emission associated to the parallel CaI(X 2Σ+ ← B 2Σ+) emission led into a strong polarization of the product rotational angular momentum. The comparison of the product rotational alignment for the kinematically identical Ca(1D2, 3PJ, 1P1) + CH3 → CaI* (B2Σ+) + CH3 reaction system showed that the CaI rotational polarization diminishes in the 3PJ1D21P1 sequence, e.g. as the reaction exothermicity increases. In addition the degree of polarization associated with other emission bands as for example CaI(X 2Σ+ ← A 2Π1/2) indicates the presence of a parallel transition which was been interpreted as mixing of Hund's case (a) and (c) appropriate for this heavy CaI diatom produced with a high rotational excitation.  相似文献   


10.
A method was developed to improve the precision of inductively coupled plasma quadrupole mass spectrometry (ICP-QMS) for the determination of boron isotope ratios (11B/10B) in various environmental materials including seawater. This approach is based on the common analyte internal standardization (CAIS) chemometric algorithm. The sample solution obtained after digestion is spiked with lithium, and both 7Li/6Li and 11B/10B values are measured using long-counting periods (20 min). The CAIS algorithm corrects the measured 11B/10B values for (a) statistical fluctuations resulting from short-term noise; (b) drift in 11B-to-10B ratio as a result of long-term deviation in instrumental parameters likely to occur during long counting times; (c) change in 11B-to-10B ratio caused by variation in matrix elements concentrations; and (d) drift in mass bias correction factor. Comparing boron isotopic ratios in seawater measured by conventional and the new isotope ratio methods validates the procedure. A synthetic isotopic mixture of boron SRM 951 and enriched 10B SRM 952 also was examined. The CAIS method provided a measured boron isotopic ratio precision of 0.05% R.S.D. while eliminating 5.1% matrix concentration error and 0.25% instrumental drift error.  相似文献   

11.
We present a detailed investigation of the quantum efficiency of the 1S0 and 3P0,1 levels in Pr3+ doped YF3 under VUV excitation. The quantum efficiency of the 3P0,1 level was determined by the measurement and comparison of the photon fluxes of the 1S0 → 1I6 transition around 400 nm with the visible emissions occurring from the 3P0,1 levels. It was found that already at concentrations as low as 0.01% the 3P0,1 emission quantum efficiency is only about 61%. The quenching process is most probable caused by an energy transfer cross relaxation process involving the 3P0,1 levels and the 3H4 ground state. For concentrations of 0.1%, 0.5%, 1% and 10%, the quantum efficiency was determined to be about 42%, 29%, 17%, and 0.4%, respectively. The total quantum efficiency of the visible emission (380–750 nm) under excitation at 190 nm, determined by measurements of the total photon flux, has a maximum for a Pr3+ concentration of 1%. At this value, the absorption efficiency of the 4f5d absorption bands is very high and the 3P0,1 quenching is only moderate.  相似文献   

12.
The radiative lifetimes of the b1Σ+ and a1Δ states have been evaluated by perturbation expansions including X3Σ, a1Δ, b1Σ+, 13,1Π, 23,1Π, 23Σ and 21Σ+ states. All wavefunctions result from large MRD CI calculations. The b—X transition is dominated by the parallel transition moment; it is found to be much stronger than the a—X transition. The calculated radiative lifetimes of τ(1Σ+)=18 ms, τ(1Δ)=2.2 s for NF and τ(1Σ+)=2.5–3.5 ms for NCl are in good accord with corresponding experimentally deduced values. The lifetime for the a1Δ state in NCl is found to be τ(1Δ)=1.1 s, ie. much longer than derived from a recent experiment. Its magnitude is consistent with the τ(b1Σ+)/τ(a1Δ) ratio of similar systems and with the decrease in lifetime from NF to NCl and is thus believed to be quite reliable. A detailed analysis of all contributions of the perturber states to the transition mechanism is made and comparison with the related data in SO, O2 and S2 is undertaken. The b-a transition probability dominated by the quadrupole transition is fairly constant in all the systems in the order of A = 0.013 (NF) - 0.0013 (S2) s−1.  相似文献   

13.
The phase speciation of thorium and consequences for the residence times of colloids have been examined in seawater of the Middle Atlantic Bight (MAB) and the Gulf of Mexico. Two fractions of colloidal organic matter (COM), 0.2 μm > COM1 > 1 kD and 0.2 μm > COM10 > 10 kD, were sampled using cross-flow ultrafiltration techniques and measured for their 234Th activity and organic carbon concentration. The ratios of mass concentrations of COM1 to those of suspended particulate matter were as high as 10 in the MAB and 6–34 in the Gulf of Mexico. Higher concentrations of colloids may be of great importance in the biogeochemical cycling of many particle-reactive nuclides or trace elements owing to their high specific surface area and complexation capacity. A significant fraction of 234Th in the traditionally defined “dissolved” pool was found to be associated with colloids. On average, about 10% of “dissolved” 234Th was in the colloidal fraction of sizes between 10 kDa and 0.2 μm, and 50% was in the 1 kDa-0.2 μm fraction. Values of the partition coefficients [Kc: (0.5−4) × 106 ml g−1 for Kc1 and (0.5−7) × 106 ml g−1 for Kc10] of 234Th between truly dissolved (<1 kDa) and colloidal fractions approximated those for Th-particle interactions [Kp: (0.3−10) × 106 ml g−1], indicating that colloid and suspended particle surface sites are similar. The distribution of 234Th between dissolved, colloidal, and particulate phases was broadly similar to that of organic carbon in these oceanic environments. Thus, thorium isotopes might be used as tracers of marine organic carbon cycling. Residence times of colloids derived from 234Th:238U disequilibria were consistently short, ranging from 1 to 14 days for COM10 and from 5 to 65 days for COM1, suggesting that marine colloids are highly reactive in marine biogeochemical processes. The discrepancy between apparent turnover times of colloids (1 kDa) derived from Th scavenging and 14C measurements suggest that 234Th and 14C may trace different geochemical pathways of colloids in the ocean.  相似文献   

14.
合成了1,3-丙二胺邻苯二酚钼钨手性八面体配合物(NH3CH2CH2CH2NH2)2[Mo0.4W0.6O2(C6H4O2)2],并对其进行了单晶结构解析,研究了其与ATP作用的液相NMR谱.该晶体属正交晶系,空间群为Pcan.晶胞参数a=0.7501(2)nm,b=2.3994(7)nm,c=1.2178(4)nm,Z=4.[Mo0.4W0.6O2(C6H4O2)2]2-的配位几何构型为手性八面体,晶体为外消旋体.配位阴离子中MoW中心金属离子除了与两个端基O配位形成cis-MO键外,同时还分别与两个邻苯二酚配位基团的的氧原子配位,形成4个M-Ob(M=Mo,W)键,构成两个五元环.利用1HNMR,13CNMR,31PNMR以及1H-15NHMBC对标题配合物及其与ATP在D2O溶剂中的作用进行了研究,发现标题配合物的MoW中心金属离子在纯D2O溶剂中被还原成+5价,但与ATP混合后转化为+6价,且与原配位基邻苯二酚发生解离.解离后的[MO2]2+最大可能与腺嘌呤上的氨基N原子配位,而此配位可能是其抗癌抗肿瘤活性的主要作用机理之一.  相似文献   

15.
Rahman MA  Kaneco S  Amin MN  Suzuki T  Ohta K 《Talanta》2004,62(5):1047-1050
A preconcentration method for silver in environmental waters involving adsorption on a tungsten wire, followed by electrothermal atomic absorption spectrometry with a tungsten tube atomizer is described. The optimal immersing time was 90 s. The best pH for the adsorption of silver was 3. Under the optimal conditions, the detection limit for silver by the tungsten wire preconcentration method was 5.0 ng l−1 (3S/N) and the relative standard deviation was 8.2%. The effects of large amounts of concomitants on the preconcentration of silver were evaluated. Even though 103- to 104-fold excess of matrix elements existed in water, the silver response was not significantly affected by the matrix elements. The method with preconcentration on a tungsten wire was applied to the determination of silver in waters and proved to be sensitive, simple, and convenient. This adsorption method can be utilized in in situ sampling of ultra-trace silver in environmental samples (waters). Furthermore, after sampling it is easy to carry and store the tungsten wire without contamination for a long time.  相似文献   

16.
Large-scale MRD CI calculations assign to AlP the ground state X 3Σ (9σ22) and a close-lying state 1 3Π (9σ3π3) (Te = 0.08 eV). Up to transition energies of 2.0 eV, other states are described by the configurations 9σ3π3 (11Π), 8σ24 (1 1Σ+), 9σ22 (1 1Δ and 2 1Σ+) and 9σ3π24π (1 5Π). The 2 3Π state, located at ≈ 2.30 eV, shows a shallow double minimum. Numerous perturbations are expected to induce predissociation upon 2 3Π. Multiplets arising from the occupation 8σ234π are clustered in the 3.25–3.50 eV region. Quintet states with the configuration 8σ9σ3π34π are bound, with Te values (in eV) of 3.80 (1 5Σ+), 4.44 (1 5Δ) and 4.88 (3 5Σ), respectively. The 9σ → 4s Rydberg members 5Σ and 3Σ lie in the 4.58–4.72 eV energy region. The first ionization potential (ionization to X4Σ of AlP+, 9σ → ∞) is estimated to be 7.65 eV. Ionization to the 1 2Σ and 1 2Π states of AlP+ is suggested to occur between 8.0 and 8.8 eV. The dipole moments of X 3Σ, 1 1Δ and 2 1Σ+ are close to 1.0 D, whereas the 1 1Σ+ state has μ = 3.49 D; 1 3Π and 1 1Π have dipole moments from 2.45 to 2.91 D. All low-lying states show a polarity Al+P. Finally, the electronic structure and transition energies of AlP are compared with those of the isoelectronic species BN, AIN, and SiP+.  相似文献   

17.
The perphenylmetallocene complexes (η5-C5Ph5)2W (1), [(η5-C5Ph5)2W]+I3 (1+I3), (η5-C5Ph5)2Mo (2) and [(η5-C5Ph5)2Mo]+I3 (2+I3) have been prepared. Hydrogenation of 1 in THF produces (η5-C5Ph5)2WH2 (4), while (η5-C5Ph5)2WHCl (3) is afforded in 1,2-dichloroethane solvent. Carbonylation of 1 produces (η5-C5Ph5)2W(CO) (5). Treatment of 1 with the strong acid CF3SO3H leads to the dicationic species [(η5-C5Ph5)2W]+2[CF3SO3]2 (1+2Tf2) after crystallization. The structures of 2+I3 and 1+2Tf2 have been determined by an X-ray diffraction study. The magnetic susceptibility study indicates a 3E2g ground-state for 1 and 2, and a 4A2g ground-state for 1+ and 2+.  相似文献   

18.
尖吻蝮蛇毒抗凝血因子(ACF)分子中有两个钙离子结合位点,钙离子对ACF的内源荧光有增强作用,稀土离子(Nd3+,Sm3+,Eu3+,Gd3+和Tb3+)能取代ACF分子中的钙离子,并对ACF的内源荧光有不同程度的猝灭作用,其中Tb3+接受ACF分子中Trp残基传递的能量后,特征荧光增强.稀土离子与ACF荧光滴定表明,ACF分子中有两个稀土离子结合位点,稀土离子和钙离子在ACF分子中两个结合部位是共同的竞争结合部位.ACF与不同稀土离子之间有相近的表观结合常数K1或K2.Tb3+与RE3+(RE=Nd,Sm,Eu或Gd)间线性自由能关系表明,稀土离子与ACF结合时,没有明显的空间效应.ACF分子中的两个结合位点在结构上都有较大的柔性,这种结构柔性为钙离子在ACF与活化凝血因子X的结合反应中起到的促进作用提供了结构基础.  相似文献   

19.
Three novel flame retardants containing both phosphorus and silicon elements in their structures,including[(1,1,3,3- tetramethyl-1,3-disiloxanediyl)di-2,1-ethanediyl]bis(diphenylphosphine oxide)(FR-1),[(2,4,6,8-tetramethylcyclotetra-siloxane -2,4,6,8-tetrayl)tetra-2,1-ethanediyl]tetrakis[diphenylphosphine oxide](FR-2) and 1,3,5,7,9,11,13,15-octakis(di-phenylphosphine oxide-2,1-ethanediyl)pentacyclo[9.5.1.13,9.l5,15.17,13]octasiloxane(FR-3) were synthesized by a convenient pathway from the reaction of diphenylphosphine oxide(DPPO) and vinyl-terminated siloxanes under the catalysis of triethylborane. The chemical structures of the target compounds were confirmed by nuclear magnetic resonance(1H NMR,13C NMR,29Si NMR and 31P NMR),matrix-assisted laser desorption/ionization time-of-flight mass spectrometry(MALDI-TOF-MS) and Fourier transform infrared(FT IR) measurements.Thermogravimetric analysis(TGA) results indicated that the new flame retardants possessed good thermal stability both in nitrogen and in air.FR-3 containing polyhedral oligosilsesquioxanes(POSS) moiety exhibited the best thermal properties with a 10%weight loss temperature>400℃ and a residual weight ratio>39%at 700℃ .  相似文献   

20.
2,2-Dichloro-1,3-bis(trimethylsilyl)-1,3,2-diazastanna-[3]ferrocenophane (3) reacts with lithium alkynides LiCCR1 to give the corresponding di(alkyn-1-yl)tin derivatives 4a (R1=tBu) and 4b (R1=SiMe3). 1,1-Organoboration of 4 with triethylborane affords the spirotin compounds 5 which contain both a ferrocenophane and a stannacyclopentadiene ring. The crystal structure of 5b was determined by X-ray analysis. The compounds 4 and 5 were characterised in solution by multinuclear magnetic resonance (1H-, 11B-, 13C-, 15N-, 29Si-, 119Sn-NMR), using pulsed field gradients in HMBC experiments for the 1H detected 15N- and 119Sn-NMR signals. The compound 5b was also studied by solid-state 13C, 29Si and 119Sn MAS NMR in order to correlate liquid and solid-state NMR data with the structural evidence.  相似文献   

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