125 resultados para 1.95 GeV Kr ions


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本文简要介绍了快重离子在固体材料,特别是在高分子材料和团簇材料中引起强电子激发效应研究的发展历史、研究现状和基本理论。重点描述了在兰州重离子加速器(HIRFL)上完成的2.1 GeV Kr离子辐照聚碳酸酷CPC)膜的实验和辐照样品的傅立叶变换红外光谱(FTIR )和紫外/可见光谱(UVIVIS )分析。FTIR分析结果表明,高能Kr离子在PC膜中引起的辐照效应主要是键的断裂和材料的降解。随着电子能损和辐照剂量的增大,材料逐渐碳化,同时有炔基生成。在UVNIS中,380, 450, 500nm波长处的吸光度之差(A-A_0)与剂量近似成线性关系,与电子能损呈确定的指数关系(指数分别为1.69,1.86和2.02);与电子能量沉积密度也近似成指数关系。描述了在HIRFL上完成的2.0GeV Xe离子辐照C_(60)薄膜的实验和辐照样品的FTIR谱、拉曼谱(Raman)和X射线衍射谱(XRD)分析。分析结果表明:2.0 GeV Xe离子辐照C60薄膜引起的损伤过程主要取决于强电子激发,在特定电子能损处,损伤的部分恢复是由于强电子激发的退火效应引起的。快重离子辐照产生的物理化学改性不仅与离子的电子能损有关,还与离子的速度有关。在同样的电子能损下,速度越小,产生的效应就越明显。

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AIM: To determine whether trichobitacin, a novel ribosome-inactivating protein purified from the root tubers of Trichosanthes kirilowii, possesses the anti-HIV activity. METHODS: The inhibition of syncytial cell formation induced by human immunodeficiency virus type 1 (HIV-1),was determined under microscope, reduction of HIV-1 p24 antigen expression level was measured by ELISA, and decrease in numbers of HIV-1 antigen positive cells in acutely and-chronically infected cultures were detected by indirect immunofluorescence assay. RESULTS: Trichobitacin Was-found to greatly suppress syncytial cell formation induced by HIV-1 and to markedly reduce both expression of HIV-1 p24 antigen and the number of HIV antigen positive cells in acutely but not chronically HIV-1 infected culture. The median inhibitory concentration (IC50) in inhibition of syncytial cell formation and HIV antigen positive cells were 5 mu g.L-1 (95 % confidence limits: 1.3 - 20 mu g.L-1) and 0.09 mg.L-1 (95 % confidence limits: 0.011 - 0.755 mg.L-1), respectively. CONCLUSION: Trichobitacin is a novel ribosome-inactivating protein with anti-HIV-l activity.

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The lattice damage accumulation in GaAs and Al0.3Ga0.7As/GaAs superlattices by 1 MeV Si+ irradiation at room temperature and 350-degrees-C has been studied. For irradiations at 350-degrees-C, at lower doses the samples were almost defect-free after irradiation, while a large density of accumulated defects was induced at a higher dose. The critical dose above which the damage accumulation is more efficient is estimated to be 2 x 10(15) Si/cm2 for GaAs, and is 5 x 10(15) Si/cm2 for Al0.8Ga0.7As/GaAs superlattice for implantation with 1.0 MeV Si ions at 350-degrees-C. The damage accumulation rate for 1 MeV Si ion implantation in Al0.3Ga0.7As/GaAs superlattice is less than that in GaAs.

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During the last years FOPI has developed a new ToF system as an upgrade of the existing detector based on Multi-strip Multi-gap Resistive Plate Chambers (MMRPCs). The intention is to increase the charged Kaon identification up to a laboratory momentum of 1 GeV/c and to enhance the azimuthal detector granularity. The new ToF barrel has an active area of 5 m(2) with 2400 individual strips (900 x 1.6 mm(2)) [A. Schuttauf, et al., Nucl. Phys. B 158 (2006) 52] which are read out on both sides by a custom designed electronics [M. Ciobanu, et al., IEEE Trans. Nucl. Sci. NS-54 (4) (2007) 1201; K. Koch, et al., IEEE Trans. Nucl. Sci. NS-52(3) (2005) 745]. To reach the envisaged goal a time resolution of 100 ps is needed, at a flight path of 1-1.3 m. Due to the rare production of the K- at SIS energies the efficiency of the MMRPCs has to be above 95%. We report on measurements with the detectors and electronics from the mass production line. For this purpose we used a proton beam at 2.0 and 1.25 GeV, at rates between 0.1 and 5 kHz/cm(2) to determine the timing, efficiency and rate capability of the MMRPCs

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With an effective Lagrangian approach, we analyze several NN -> NN pi pi channels by including various resonances with mass up to 1.72 GeV. For the channels with the pion pair of isospin zero, we confirm the dominance of N*(1440) -> N sigma in the near-threshold region. At higher energies and for channels with the final pion pair of isospin one, we find large contributions from N*(1440) -> Delta pi, double-Delta, Delta(1600) -> N*(1440)pi, Delta(1600) -> Delta pi and Delta(1620) -> Delta pi. There are also sizable contributions from Delta -> Delta pi, Delta -> N pi, N -> Delta pi, and nucleon pole at energies close to the threshold. We give a good reproduction to the total cross sections up to beam energies of 2.2 GeV except for the pp -> pp pi(0)pi(0) channel at energies around 1.1 GeV and our results agree with the existing data of differential cross sections of pp -> pp pi(+)p pi(-), pp -> nn pi(+)pi(+), and pp -> pp pi(0)pi(0) which are measured at CELSIUS and COSY.

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Vacancy-type defects are introduced into magnesium aluminate spine] (MgAl2O4 (1 1 0)) by Ar-ions implantation, and then Ag-ions are implanted into the depth rich in vacancy-type defects. The ultraviolet-visible spectrometry (UV-VIS) and positron annihilation spectroscopy (PAS) are used to study the influence of vacancy-type defects on nucleation of Ag nanoparticles. After introduction of vacancy-type defects the pronounced increase of surface plasmon resonance (SPR) absorbance intensity indicates that defects enhance the nucleation of Ag nanoparticles. The PAS results reveal that vacancy-type defects provide pre-nucleating centers for Ag nanoparticles nucleation and growth. (C) 2010 Elsevier B.V. All rights reserved.

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Two new compounds, [CoL2(H2O)(2)](NO3)(2). 8H(2)O (1) and [CoL(H2O)(2)(CH3CO2)(2)]. H2O (2), were obtained from self-assembly of the corresponding metal salts with 1,1'-(1,4-butanediyl)bis(benzimidazole) (L). In 1, each cobalt ion is coordinated to four nitrogen atoms from four molecules of L, and to two water molecules. Metal ions are bridged by L ligands to form infinite (4, 4) networks that contain 44-membered rings. The (4, 4) networks of 1 stack in a parallel fashion, resulting in the formation of large channels in the material. In 2, each cobalt ion is coordinated to two N atoms from two L molecules, two water molecules and two carboxylate O atoms from two acetate anions. Each L molecule is coordinated to two cobalt ions, acting as a bridging ligand as in 1. The bridged cobalt ions form an infinite zigzag chain structure.

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以1,4-萘醌为原料,经溴化、氰化、烷基化合成了1,4-二丙氧基-2,3-二氰基萘,用SiemensP4四圆衍射仪测得了晶体结构。合成方法简便,反应时间短,产率高。

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趋磁细菌(Magnetotactic bacteria)的研究是国际微生物学研究热点之一。趋磁细菌体内含有纳米单磁畴的氧化铁/硫化铁(Fe3O4或Fe3S4)晶体,称为磁小体。由于趋磁细菌营养条件要求苛刻,在环境中需要微好氧条件,且营养类型属于化能自养,使得培养趋磁细菌时常遇到问题。 本研究首先通过正交试验优化趋磁细菌AMB-1菌株培养条件,在培养条件铁源为奎尼酸铁0.02 mmol/L,装瓶量75% ,pH值6.7,温度25 ℃时,AMB-1 OD600达到0.440(1.166×109 cells/ml)。同时运用磁收集传代法,使带有磁小体的AMB-1细胞比例占95%以上(Cmag值稳定在1.9-2.0)。 在AMB-1具有较好的生物量,同时又具有较好的含磁小体细胞比例后,研究磁小体的变化过程。通过透射电镜观察磁小体变化过程,发现培养24 h细菌体内已有较小晶体形成(平均27 nm,n=188)且沿长轴分布;48 h晶体长大(平均43 nm,n=203)且形成分段链沿长轴排列;72 h晶体进一步成熟(平均50 nm,n=191)仍以分段链沿长轴排列;随后细菌逐渐衰亡磁小体变小,168 h可见部分自溶细菌中仍有磁小体链(平均37 nm,n=186);192 h细菌自溶磁小体链(平均33 nm,n=184)分散到环境中。 通过透射电镜在细胞水平上研究趋磁细菌细胞分裂时发现,磁小体在细菌分裂时采用两种分离方式:一种为磁小体分配到两个子细胞;另一种为磁小体只分配到一个子细胞。无磁小体的子细胞,在随后的生长过程又分为两种情况:一种为细胞逐渐产生磁小体,另一种为不再产生磁小体。这种现象的发现,解释了随着传代次数的增多,细菌磁性有所下降的原因(Cmag值降低)。 在对趋磁细菌磁小体合成机制的研究中,常使用基因敲除的办法获得缺陷型,并与野生型对比进行研究。但是,利用基因敲除获得缺陷型不仅操作繁琐并且所得缺陷型不稳定。本研究利用特殊的磁富集传代法,先将带有磁小体的菌体收集并连续传代,筛选获得了高磁菌株;利用这种方法,收集不含磁小体的菌体并连续传代,筛选获得了无磁菌株。 趋磁细菌磁小体在医疗、环保等领域具有广阔应用价值,但是目前由于趋磁细菌难以大规模培养,并且磁小体纯化存在成本高等原因,将磁小体真正实际应用尚有一段距离。通过研究磁小体在趋磁细菌中的变化过程发现,AMB-1菌株在培养192 h后自溶,并且磁小体随着细胞的破碎释放到环境中去。

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在94mm×94mm方截面激波管上,入射激波马赫数为1.60~1.95内开展了汽油/空气可燃混合气体在激波聚焦方式下的点火实验.当汽油/空气混合比处于化学恰当比附近,激波马赫数为1.69~1.95的激波聚焦能够成功地引燃汽油/空气的可燃混合气体,而当入射激波马赫数低于1.69时,同样条件下的汽油/空气混合气体不能被点燃.流场的纹影照片显示,与未燃状态相比,汽油/空气可燃混合气体被引燃后的反射激波波面变宽.

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MeV An irradiation leads to a shape change of polystyrene (PS) and SiO2 particles from spherical to ellipsoidal, with an aspect ratio that can be precisely controlled by the ion fluence. Sub-micrometer PS and SiO2 particles were deposited on copper substrates and irradiated with Au ions at 230 K, using an ion energy and fluence ranging from 2 to 10 MeV and 1 x 10(14) ions/cm(2) to 1 x 10(15) ions/cm(2). The mechanisms of anisotropic deformation of PS and SiO2 particles are different because of their distinct physical and chemical properties. At the start of irradiation, the volume of PS particles decrease, then the aspect ratio increases with fluence, whereas for SiO2 particles the volume remains constant. (C) 2008 Elsevier B.V. All rights reserved.

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Human serum albumin adsorption onto gold surfaces was investigated by electrochemical and ellipsometric methods. Albumin adsorption onto gold was confirmed by the change of the open circuit potential of gold and by the ellipsometric parameter variation during albumin immobilization. In both experiments the parameters reached stable values within 10-15 min. The albumin adsorption layer thickness measured with the ellipsometer was about 1.5 nm. The adsorption of albumin Under applied potential was also investigated and it was found that both positive and negative applied potential promote albumin adsorption. Changes in the optical parameters of bare gold and albumin adsorbed onto gold surface under applied potential were investigated with in Situ ellipsometry. The similarity and reversibility of the optical changes showed that adsorbed albumin was stable on the gold surface Under the applied potential range (-200-600 mV). The cyclic voltammograms of K3Fe(CN)(6) on the modified gold surface showed that albumin Could partly block the oxidation and reduction reaction. (C) 2004 Elsevier Inc. All rights reserved.

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对所有多细胞生物体而言,其个体发育均涉及由初始的单个细胞开始,经过在时间和空间上细胞有序地增殖、凋亡、分化、迁移等诸多过程,并最终生成物种特异的生物模式.对模式形成的机制的探讨一直是发育生物学的中心课题.目前已就这个问题积累了大量的分子生物学、生物化学、数学、力学等多学科的研究数据并提出了一些模式形成的理论,然而,迄今为止,模式形成的真正机制仍然很不清楚而需进一步的深入探索.本文简要介绍了生物发育过程中模式形成的一些典型的力学模型,重点在于力学模型的建立及其模型本身的介绍,而对其数值模拟和具体应用很少涉及.

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为了更深入地了解湍流的物理过程,综述了各向同性湍流的基础问题。在评述了Kolmogorov能谱及能量级串过程后,深入讨论了Kolmogorov局部各向同性假设。接着综述了涉及能量传递的以及包括三元组相互作用的各向同性湍流相互作用尺度的详细物理过程。还讨论了惯性区、自相似性以及小尺度对大尺度各向异性的响应和末期衰减过程。之后为了举例说明这些论点,详细讨论了根据各向同性湍流直接模拟得到的结果(包括对亚格子模型的讨论)。最后,综述了各向同性湍流的自保持性,并展望了今后的研究方向。