369 resultados para MEV LI-6 IONS


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We have studied the excitation and dissociation processes of the molecule W(CO)(6) in collisions with low kinetic energy (3 keV) protons, monocharged fluorine, and chlorine ions using double charge transfer spectroscopy. By analyzing the kinetic energy loss of the projectile anions, we measured the excitation energy distribution of the produced transient dications W(CO)(6)(2+). By coincidence measurements between the anions and the stable or fragments of W(CO)(6)(2+), we determined the energy distribution for each dissociation channel. Based on the experimental data, the emission of the first CO was tentatively attributed to a nonstatistical direct dissociation process and the emission of the second or more CO ligands was attributed to the statistical dissociation processes. The dissociation energies for the successive breaking of the W-CO bond were estimated using a cascade model. The ratio between charge separation and evaporation (by the loss of CO+ and CO, respectively) channels was estimated to be 6% in the case of Cl+ impact. (C) 2011 American Institute of Physics. [doi: 10.1063/1.3523347]

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Aims. We determine branching fractions, cross sections and thermal rate constants for the dissociative recombination of CD3CDOD+ and CH3CH2OH2+ at the low relative kinetic energies encountered in the interstellar medium. Methods. The experiments were carried out by merging an ion and electron beam at the heavy ion storage ring CRYRING, Stockholm, Sweden. Results. Break-up of the CCO structure into three heavy fragments is not found for either of the ions. Instead the CCO structure is retained in 23 +/- 3% of the DR reactions of CD3CDOD+ and 7 +/- 3% in the DR of CH3CH2OH2+, whereas rupture into two heavy fragments occurs in 77 +/- 3% and 93 +/- 3% of the DR events of the respective ions. The measured cross sections were fitted between 1-200 meV yielding the following thermal rate constants and cross-section dependencies on the relative kinetic energy: sigma(E-cm[eV]) = 1.7 +/- 0.3 x 10(-15)(Ecm[eV])(-1.23 +/- 0.02) cm(2) and k(T) = 1.9 +/- 0.4 x 10(-6)(T/300)-0.73 +/- 0.02 cm(3) s(-1) for CH3CH2OH2+ as well as k(T) = 1.1 +/- 0.4 x 10(-6)(T/300)(-0.74 +/- 0.05) cm(3) s(-1) and s(Ecm[eV]) = 9.2 +/- 4 x 10(-16)(Ecm[eV])-1.24 +/- 0.05 cm(2) for CD3CDOD+

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本论文以在微生物油脂生产中较具潜力的粘红酵母为材料,利用兰州近代物理研究所重离子研究装置(HIRFL)产生的80 MeV/u碳离子束对产油菌株粘红酵母进行辐照诱变, 采用含有脂肪酸合成酶抑制剂cerulenin的培养基进行高产油脂突变株的初选, 并通过磷酸香草醛反应和氯仿甲醇抽提法对初筛菌株油脂含量进行分析,复选出油脂产量和质量都有较大提高的突变菌株,并对其产油条件进行优化,以期获得一些其它诱变方法难以获得的高产油脂微生物突变株,大力开发离子束辐照技术在解决能源危机中的应用。通过本论文的实验研究,得到了以下初步结果 : 1.液体培养基中,粘红酵母菌在接种后的40h-80h处于对数生长期,此时菌体的生长繁殖比较旺盛,活力最佳,为辐照诱变的最适时期。辐照后,不同来源的菌株对重离子辐射的敏感性有所不同,然而其存活趋势却大致相当。菌体的存活率都呈现出随辐照剂量的增加先减小后增加,再减小的马鞍型剂量-效应曲线。 2.cerulenin对酵母细胞的生长具有较好的抑制作用,浓度为8.96×10-6 mol/L时,抑制率达98%以上,可作为高产油脂粘红酵母菌的筛选浓度。通过磷酸香草醛反应法和氯仿-甲醇抽提法对初筛菌体油脂含量进行定量分析,结果表明初筛菌株的正突变率达66%以上。该方法快速方便,是一种较为理想的高产油脂酵母菌的筛选方法。通过这些方法,筛选出了2株油脂含量明显高于对照的突变株。 3.经实验发现,菌体培养物与磷酸香草醛试剂反应后在530nm的光吸收与氯仿-甲醇抽提法所测得的菌体油脂含量成正比,其标准曲线方程为y=38.2257x+0.67314,R2为0.995,从而建立起一种方便快捷的油脂定量测量方法,有望实现自动化分析。 4.通过对影响粘红酵母菌生长和油脂合成的几个主要因素(葡萄糖浓度、碳氮比、接种量、培养时间、温度、PH值)的初步探讨研究,得出了粘红酵母突变株的最佳产脂条件为: 葡萄糖浓度10%,碳氮比40:1,接种量10%,温度28℃,PH=5.0,培养时间为6天

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本文简要叙述了快重离子在固体材料,特别是聚合物材料中引起的强电子激发效应研究的基本理论、发展历史和研究现状。描述了在兰州重离子加速器上完成的25 MeV/u 86Kr离子辐照叠层聚对苯二甲酸乙二醇酯膜(PET)和聚碳酸酯(PC)膜的实验及结果分析。应用傅立叶红外变换光谱(FT-IR)及X-射线衍射分析(XRD)方法研究了在不同电子能损及不同注量辐照条件下,高能Kr离子在聚合物PET和PC潜径迹中引起的的损伤效应。结果表明:高能Kr离子在聚合物PET、PC膜引起的损伤主要是由于辐照引起的断键及键的重组产生的官能团的降解及非晶化过程,损伤截面存在电子能损阈值,且与官能团的结构有关。 对PET的傅立叶红外变换光谱分析结果给出,电子能损为7.25 keV/nm时,对应官能团吸收峰794 cm-1, 849 cm-1, 1021 cm-1, 1341 cm-1, 1410 cm-1, 1505 cm-1,的损伤截面半径分别为:3.63 nm, 4.70 nm, 4.58 nm, 3.54 nm, 5.17 nm, 5.32 nm。X-射线衍射分析结果表明,PET的非晶化转变截面随离子注量和电子能损的增大而增加,(100)衍射峰的相对强度I/I0随离子注量的增加而指数衰减,对应电子能损为6.62, 6.93, 7.25 keV/nm,其相应的非晶化半径分别为4.86, 5.64, 6.77 nm。 对PC的傅立叶红外变换光谱分析表明,当电子能损比较小,大多数官能团的红外吸收无明显变化,直到当辐照注量为2×1012 ions/cm2 且电子能损比较大时,其绝对吸收强度才发生明显的改变。电子能损为6.37 keV/nm 时,对应官能团吸收峰为519 cm-1, 605 cm-1, 724 cm-1, 1014 cm-1,其损伤截面分别为:13.12, 45.40, 50.21, 56.28 nm2

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本论文共由两部分组成。第一部分描述了多丝正比室的研制过程。第二部分研究了中能区25MeV/u ~(40)Ar + ~(93)Nb反应中轻粒子发射时间的测量。本论文所研制的多丝正比室灵敏面积为5cm * 5cm。阳极丝由10μm的镀金钨丝组成,丝与丝之间的间距为0.5mm。工作气体为正庚烷,采用感应信号重心读出方法。调试了工作气压在25Torr左右、工作电压~1400v条件下多丝室的工作状态,结果表明该工作条件下,多丝正比室并未工作于正比状态下,须适当增加工作电压和工作气压才能得到较好的位置分辨。并且提出进一步的改进建议。第二部分利用小相对角度内的两粒子关联测量,研究了中能区25MeV/u ~(40)Ar + ~(93)Nb反应中高激发核衰变产生的轻粒子的发射时标。轻粒子发射时间随能量的变化很大,从低能粒子的约500fm/c变化至高能粒子的50fm/c,表明高能粒子来自于热核的早期发射,包含有前平衡发射的粒子,而低能粒子来自于平衡热核的发射。随着入射能的升高和激发能的增加,热核的寿命及其发射时标变短。轻粒子时空演化表明,发射源的核物质密度对轻粒子关联函数的影响较大,尤其是对于发射时间较(τ ≤ 100fm/c)的高能粒子的关联函数,这一影响随着粒子能量降低而减弱。在发射时间较长(τ ≤ 200fm/c)时,这种影响几乎消失。另外随着实验室系角度的增加,平衡发射成分增加,相应地提取的轻粒子的发射时间变长。

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HIRFL is a tandem cyclotron complex for heavy ion. On the beam line between SFC and SSC, there is a stripper. Behind it, the distribution of charge states of beam is a Gauss distribution. The equilibrium charge state Q_0 is selected by 1BO2(a 50° dipole behind the stripper) and delivered to SSC. One of two new small beam line (named SLAS) after 1B02 will be builded in or der to split and deliver the unused ions of charge states (Q_0 ± n) to aspecific experimental area. Q_0 ± n ions are septumed and separated from initial(Q_0) ion beam by two septum magnets SM1, SM2. The charge state selected by SM1 will be Q_0 ± 1(6 ≤ Q_0 < 17), Q_0 ± 2(17 ≤ Q_0 < 33) and Q_0 ± 3 (Q_0 ≥ 33) forming a beam in one of the two possine new beam line with the stripping energy of (0.2 to 9.83 Mev/A), an emittance of 10π mm.mrad in the two transverse planes and an intensity ranging from 10~(11) pps for z ≤ 10 to some 10~5 pps for the heaviest element. Behind SM2, a few transport elements (three dipoles and seven qudrupoles) tra nsport Q_0 ± n beam to target positions T1, T2 (see fig. 1) and generate small beam spots (φ ≤ 4mm, φ ≤ 6mm). The optics design of the beam line has been done based on SLAC-75 (a first and second - order matrix theory). beam optics calculation has been worked out with the TRANSPORT program. The design is a very economical thinking, because without building a new accelerator we can obtain a lower energy heavy ion beam to provide for a lot of atomic and solid state physical experiments

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锂同位素的结构性质,特别是滴线核 ~(11)Li的异常特性,目前微观机制并不很清楚。本文系统地研究了锂同位素基态和低位态的性质,包括基态结合能、能谱、电磁矩和电磁跃迁性质、及β衰变性质,发现~6Li核基态的四极矩敏感地依赖于相互作用力中的张量力分量,~6Li、~7Li和~8Li核的第一激发态电磁跃迁几率增大,呈现集体性,可能是由集团结构所致,对远离核~9Li的某些态需要考虑sd-shell组态侵入的影响。在~(6-9)Li核性质系统研究的基础上,发现滴线核~(11)Li核的结构性质仍可在壳模型框架内得到解释,平均场效应是引起其奇异性质的微观起因,对于~(10)Li核的性质仍需进一步探讨。对锂同位素引进平均场的同位旋依赖项尚需近一步研究。在3

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Cluster assisted photoionization processes of benzene, which was seeded in argon, induced by an intense 25 ns Nd-YAG laser has been studied by means of time-of-flight mass spectrometry. At the laser intensity of 10(11) W/cm(2), multicharged ions Cq+ (q = 2-3) with kinetic energy up to 150 eV were observed in the mass spectra. Strong evidences Support that these ions are formed in the Coulomb explosion of multicharged benzene cluster ions. (C) 2004 Elsevier B.V. All rights reserved.

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Isolated transition metal ions/oxides in molecular sieves and on surfaces are a class of active sites for selective oxidation of hydrocarbons. Identifying the active sites and their coordination structure is vital to understanding their essential role played in catalysis and designing and synthesizing more active and selective catalysts. The isolated transition metal ions in the framework of molecular sieves (e.g., TS-1, Fe-ZSM-5, and V-MCM-41) or on the surface of oxides (e.g., MoO3/Al2O3 and TiO2/SiO2) were successfully identified by UV resonance Raman spectroscopy. The charge transfer transitions between the transition metal ions and the oxygen anions are excited by a UV laser and consequently the UV resonance Raman effect greatly enhances the Raman signals of the isolated transition metal ions. The local coordination of these ions in the rigid framework of molecular sieves or in the relatively flexible structure on the surface can also be differentiated by the shifts of the resonance Raman bands. The relative concentration of the isolated transition metal ion/oxides could be estimated by the intensity ratio of Raman bands. This study demonstrates that the UV resonance Raman spectroscopy is a general technique that can be widely applied to the in-situ characterization of catalyst synthesis and catalytic reactions. (C) 2003 Elsevier Science (USA). All rights reserved.

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The effect of iron promoter on the catalytic properties of Rh-Mn-Li/SiO2 catalyst in the synthesis Of C-2 oxygenates from syngas was investigated by means of the following techniques: CO hydrogenation reaction, temperature-programmed reduction (TPR), temperature-programmed desorption and reaction of adsorbed CO (CO-TPD and TPSR) and pulse adsorption of CO. The results showed that the addition of iron promoter could improve the activity of the catalysts. Unexpectedly, the yield of C-2 oxygenates increased greatly from 331.6 up to 457.5 g/(kg h) when 0.05% Fe was added into Rh-Mn-Li/SiO2 catalyst, while no change in the selectivity to C-2 oxygenates was observed. However, the activity and selectivity Of C-2 oxygenates were greatly decreased if the Fe amount exceeded 1.0%. The existence of a little iron decreased the reducibility of Rh precursor, while the reduction of Fe component itself became easier. CO uptake decreased with increasing the quantity of Fe addition. This phenomenon was further confirmed by CO-TPD results. The CO-TPD and TPSR results showed that only the strongly adsorbed CO could be hydrogenated, while the weakly adsorbed CO was desorbed. We propose that Fe is highly dispersed and in close contact with Rh and Mn; such arrangements were responsible for the high yield Of C-2 oxygenates. (C) 2002 Elsevier Science B.V. All rights reserved.

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A method has been developed for the determination of interactions of metal ions and protein by using microdialysis sampling technique combined with pre-column derivation and reversed-phase ion-pair liquid chromatographic (HPLC analysis. Cu(II), Zn(II) and human serum albumin (HSA) were chosen as model metal ions and protein, respectively. The mixed solutions of metal ions and HSA with different molar ratios buffered with 0.1 M Tris-HCl containing 0.1 M NaCl at pH 7.43 were sampled with a mirodialysis probe by keeping perfusion rate at 1 mul/min and the temperature at 37 degreesC. The free concentrations of metal ions in microdialysates were assayed by precolumn derivatization with meso-tetra(4-sulfophenyl)-porphyrin (TPPS4) followed ion-pair HPLC analysis. The recovery (R) of microdialysis sampling was measured in vitro under similar conditions as 65.74% for Cu(II), 70.45% for Zn(II) with R.S.D. below 3.2%. The primary binding constants and number of binding site estimated by the Scatchard plot analysis are 5.04 x 10(6) M-1 and 0.85 for Cu(II), and 9.87 x 10(6) M-1 and 1.10 for Zn(II), respectively. The competition of Cu(II) and Zn(II) at the second binding site on HSA was investigated, and it was observed that there is a second site on HSA to bind Cu(II) and Zn(II), the affinity of Cu(II) is stronger than that of Zn(II) to this second site of HSA. (C) 2001 Elsevier Science B.V. All rights reserved.

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A method has been established to study the competing binding of metal ions with protein by a combined technique of microdialysis with high performance liquid chromatography (HPLC). Ni2+, Cd2+, Zn2+, Cu2+ and human serum albumin (HSA) were chosen as model metal ions and protein. The experimental results show that Ni2+ and Cu2+ share a common primary binding site on HSA, and Zn2+ and Cd2+ share a different common primary binding site from them, but there is a common multi-metal binding site for all of those four metal ions. This method show advantages of fast sampling, easily to be operated and especially to be useful when ideal spectroscopic probes are not available for the study of interaction between protein and metal ions.