75 resultados para MEV RANGE 10-100

em Chinese Academy of Sciences Institutional Repositories Grid Portal


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把QMD模型扩展至10~100MeV/A能区,研究了该能区的重离子碰撞,并仔细检验了初始核在基态时传播的稳定性条件。~(40)Ca+~(40)Ca系统,在10 ~ 100MeV/A能区范围内研究了重离子反应机制随入射能量及碰撞参数的演化情况。我们发现,反应机制随能量的变化并不是突然的跃迁,而是一个连续的变化过程,不同的反应机制可以同时存在并发生竞争。在中心碰撞时,反应机制从全融合发展至非全融合,最后演化至碎裂机制。在周连碰撞时,随着入射能量的增加,根据我们提出的关于深部非弹碰撞和参加者-旁观者质量分布的判据,反应机制的可能变化趋势为从非完全融合或深部非弹碰撞到参加者-旁观者,最后发展至碎裂反应。我们知道,目前还没有人用QMD模型来研究过渡能区DIC机制的基本特征,我们还对~(20)(25Mev/A)+~(20)Ne系统周边碰撞时DIC机制的基本特征作了研究,计算结果表明:在中能区,DIC机制仍然存在,同时,在质量分布、旋转效应及能量损失方面具有低能时相同的特征,但与低能DIC的明显差别在于,出射的中间质量碎片已成为质量分布的主要部分,出射的轻粒子数目也相对增多。当碰撞参数小于7fm时,这里存在着不同反应机制的共存及竞争。根据质量分布随时间的演化情况,我们发现,中间质量碎片主要是由动力学过程中平均场涨落引起的动力学不稳定性造成的,统计衰变也贡献较小的一部分。由粗糙估计可以看出,25MeV/A时~(20)Ne+~(20)Ne系统的DIC机制仍然是一个趋向于平衡过程。相又于低能区,中能区的周边碰撞显得相当复杂

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Abstract A state-of-the-art high energy heavy ion microbeam irradiation system is constructed at the Institute of Modern Physics of the Chinese Academy of Sciences. This microbeam system operates in both full current intensity mode and single ion mode. It delivers a predefined number of ions to preselected targets for research in biology and material science. The characteristic of this microbeam system is high energy and vertical irradiation. A quadrupole focusing system, in combination with a series of slits, has been designed to optimize the spatial resolution. A symmetrically achromatic system leads the beam downwards and serves simultaneously as an energy analyzer. A high gradient quadrupole triplet finally focuses a C6+ ion beam to 1 µm in the vacuum chamber within the energy range from 10 MeV/u to 100 MeV/u. In this paper, the IMP microbeam system is described in detail. A systematic investigation of the ion beam optics of this microbeam system is presented together with the associated aberrations. Comparison is made between the IMP microbeam system and the other existing systems to further discuss the performance of this microbeam. Then the optimized initial beam parameters are given for high resolution and high hitting efficiency. At last, the experiment platform is briefly introduced.

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Molecular beam epitaxy GaAs films on Si, with thicknesses ranging from 0.9-2.0-mu-m, were implanted with Si ions at 1.2-2.6 MeV to doses in the range 10(15)-10(16) cm-2. Subsequent rapid infrared thermal annealing was carried out at 850-degrees-C for 15 s in a flowing N2 atmosphere. Crystalline quality was analyzed by using Rutherfold backscattering/channeling technique and Raman scattering spectrometry. The experimental results show that the recrystallization process greatly depends on the dose and energy of implanted ions. Complete recrystallization with better crystalline quality can be obtained under proper implantation and subsequent annealing. In the improved layer the defect density was much lower than in the as-grown layer, especially near the interface.

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The piezoelastodynamic field equations are solved to determine the crack velocity at bifurcation for poled ferroelectric materials where the applied electrical field and mechanical stress can be varied. The underlying physical mechanism, however, may not correspond to that assumed in the analytical model. Bifurcation has been related to the occurrence of a pair of maximum circumferential stress oriented symmetrically about the moving crack path. The velocity at which this behavior prevails has been referred to as the limiting crack speed. Unlike the classical approach, bifurcation will be identified with finite distances ahead of a moving crack. Nucleation of microcracks can thus be modelled in a single formulation. This can be accomplished by using the energy density function where fracture initiation is identified with dominance of dilatation in relation to distortion. Poled ferroelectric materials are selected for this study because the microstructure effects for this class of materials can be readily reflected by the elastic, piezoelectic and dielectric permittivity constants at the macroscopic scale. Existing test data could also shed light on the trend of the analytical predictions. Numerical results are thus computed for PZT-4 and compared with those for PZT-6B in an effort to show whether the branching behavior would be affected by the difference in the material microstructures. A range of crack bifurcation speed upsilon(b) is found for different r/a and E/sigma ratios. Here, r and a stand for the radial distance and half crack length, respectively, while E and a for the electric field and mechanical stress. For PZT-6B with upsilon(b) in the range 100-1700 m/s, the bifurcation angles varied from +/-6degrees to +/-39degrees. This corresponds to E/sigma of -0.072 to 0.024 V m/N. At the same distance r/a = 0.1, PZT-4 gives upsilon(b) values of 1100-2100 m/s; bifurcation angles of +/-15degrees to +/-49degrees; and E/sigma of -0.056 to 0.059 V m/N. In general, the bifurcation angles +/-theta(0) are found to decrease with decreasing crack velocity as the distance r/a is increased. Relatively speaking, the speed upsilon(b) and angles +/-theta(0) for PZT-4 are much greater than those for PZT-6B. This may be attributed to the high electromechanical coupling effect of PZT-4. Using upsilon(b)(0) as a base reference, an equality relation upsilon(b)(-) < upsilon(b)(0) < upsilon(b)(+) can be established. The superscripts -, 0 and + refer, respectively, to negative, zero and positive electric field. This is reminiscent of the enhancement and retardation of crack growth behavior due to change in poling direction. Bifurcation characteristics are found to be somewhat erratic when r/a approaches the range 10(-2)-10(-1) where the kinetic energy densities would fluctuate and then rise as the distance from the moving crack is increased. This is an artifact introduced by the far away condition of non-vanishing particle velocity. A finite kinetic energy density prevails at infinity unless it is made to vanish in the boundary value problem. Future works are recommended to further clarify the physical mechanism(s) associated with bifurcation by means of analysis and experiment. Damage at the microscopic level needs to be addressed since it has been known to affect the macrocrack speeds and bifurcation characteristics. (C) 2002 Published by Elsevier Science Ltd.

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Gadolinium oxide thin films have been prepared on silicon (100) substrates with a low-energy dual ion-beam epitaxial technique. Substrate temperature was an important factor to affect the crystal structures and textures in an ion energy range of 100-500 eV. The films had a monoclinic Gd2O3 structure with preferred orientation ((4) over bar 02) at low substrate temperatures. When the substrate temperature was increased, the orientation turned to (202), and finally, the cubic structure appeared at the substrate temperature of 700 degreesC, which disagreed with the previous report because of the ion energy. The AES studies found that Gadolinium oxide shared Gd2O3 structures, although there were a lot of oxygen deficiencies in the films, and the XPS results confirmed this. AFM was also used to investigate the surface images of the samples. Finally, the electrical properties were presented. (C) 2004 Elsevier B.V. All rights reserved.

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Axisymmetric notched bars with notch roots of large and small radii were tested under large strain cyclic loading. The main attention is focused on the fracture behaviour of steels having cycles to failure within the range 1-100. Our study shows that a gradual transition from a static ductile nature to one of fatigue cleavage can be observed and characterized by the Coffin-Manson formula in a generalized form. Both the triaxial tensile stress within the central region of specimens and static damage caused by the first increasing load have effects on the final failure event. A generalized cyclic strain range parameter DELTAepsilon is proposed as a measure of the numerous factors affecting behaviour. Fractographs are presented to illustrate the behaviour reported in the paper.

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The heat transfer characteristics of China no. 3 kerosene were investigated experimentally and analytically under conditions relevant to a regenerative cooling system for scramjet applications. A test facility developed for the present study can handle kerosene in a temperature range of 300-1000 K, a pressure range of 2.6-5 MPa, and a mass How rate range of 10-100 g/s. In addition, the test section was uniquely designed such that both the wall temperature and the bulk fuel temperature were measured at the same location along the flowpath. The measured temperature distributions were then used to analytically deduce the local heat transfer characteristics. A 10-component kerosene surrogate was proposed and employed to calculate the fuel thermodynamic and transport properties that were required in the heat transfer analysis. Results revealed drastic changes in the fuel flow properties and heat transfer characteristics when kerosene approached its critical state. Convective heat transfer enhancement was also found as kerosene became supercritical. The heat transfer correlation in the relatively low-fuel-temperature region yielded a similar result to other commonly used jet fuels, such as JP-7 and JP-8, at compressed liquid states. In the high-fuel-temperature region, near and beyond the critical temperature, heat transfer enhancement was observed; hence, the associated correlation showed a more significant Reynolds number dependency.

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We studied in the laboratory the population growth rates of four cladocerans fed both with decomposed Microcystis aeruginosa and with a mixture of fresh colonial M. aeruginosa and Scenedesmus obliquus. The neonates of Diqphanosoma brachyurum and Daphnia carinata were able to develop into adults when they were fed with <64mum decomposed M. aeruginosa, while those of Moina micrura could not use decomposed M. aeruginosa. The population growth rate of the largest species, D. carinata, was less affected by the presence of fresh colonial M. aeruginosa than the other three species. D. carinata obtained the highest growth rate at a biomass level of 10 mg L-1 fresh colonial M. aeruginosa, indicating that, to some extent, it can use colonial M. aeruginosa at a size range of 64-112mum. The population growth rate of M. micrura was negatively correlated with fresh colonial M. aeruginosa within a range of 10-100 mg L-1. The population growth rates of D. brachyurum and Ceriodaphnia cornuta were remarkably decreased by fresh colonial M. aeruginosa, although no significant difference was found within the M. aeruginosa biomass range of 10-100 mg L-1 for either cladoceran. At a biomass level of 50 mg L-1 M. aeruginosa, the population growth rates of the four cladocerans positively correlated with S. obliquus biomass within a range of 0.1-5.0 mg L-1. Our results indicate that the zooplankton community under bloom condition is shaped by the quantity of both M. aeruginosa and other edible algae.

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Gadolinium oxide thin films have been prepared on silicon (100) substrates with a low-energy dual ion-beam epitaxial technique. Substrate temperature was an important factor to affect the crystal structures and textures in an ion energy range of 100-500 eV. The films had a monoclinic Gd2O3 structure with preferred orientation ((4) over bar 02) at low substrate temperatures. When the substrate temperature was increased, the orientation turned to (202), and finally, the cubic structure appeared at the substrate temperature of 700 degreesC, which disagreed with the previous report because of the ion energy. The AES studies found that Gadolinium oxide shared Gd2O3 structures, although there were a lot of oxygen deficiencies in the films, and the XPS results confirmed this. AFM was also used to investigate the surface images of the samples. Finally, the electrical properties were presented. (C) 2004 Elsevier B.V. All rights reserved.

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We propose a simple approach to generate a high quality 10 GHz 1.9 ps optical pulse train using a semiconductor optical amplifier and silica-based highly nonlinear fiber. An optical pulse generator based on our proposed scheme is easy to set up with commercially available optical components. A 10 GHz, 1.9 ps optical pulse train is obtained with timing jitter as low as 60 fs over the frequency range 10 Hz-1 MHz. With a wavelength tunable CW laser, a wide wavelength tunable span can be achieved over the entire C band. The proposed optical pulse generator also can operate at different repetition rates from 3 to 10 GHz.

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中能重离子碰撞(10-100 MeV/u)为研究热核性质提供了有力的工龄。为此我们利用HIRFL提供的46.7 MeV/u ~(12)C束轰击~(159)Tb/~(197)Au/~(209)Bi研究了线动量转移分析、出平面角分布和质量分布,实验结果的分析证实了非完全熔合核的裂变和蒸发。编写了一个Monte-Carlo统计衰变程序(SAGEE)并用于详细比较C+Au、C+Bi的实验数据,C+Tb的质量分布由统计两体发射理论(GEMINI)得到了解释。理论与实验的符合说明:通常类熔合反应方式形成了高激发的复合核,其后以统计两体衰变而退激。实验也统计了与裂变符合的γ能谱、三裂变的相对角度和相对速度分布,没有观察到GDR,对称三裂不是唯一的三裂方式。本文分析了HIRFL上其他小组的实验结果。研究了46.7MeV/u ~(12)C+~(58)Ni反应的复杂粒子发射,也研究了复杂粒子出射对用放射化学方法测量的24MeV/u ~(12)C+~(64)Cu和42MeV/u ~(12)C+~(115)In的质量产额分布的解释。GEMINI计算很好地符合了实验结果,这意味着非完全熔合反应形成的复合核的两体衰变仍是主要的发射过程。本文也简要讨论了多重碎裂过程。基于卡西尼亚卵形体裂变形状,计算了转动核的对称和非对称形变势能,用此模型得到了核的静态裂变位垒、鞍点能并与RLDM和RFRM作了比较。我们考虑了YPE核势对核表面的弥散作用以及弥散核表面对库仑能、转动惯量的影响完善了RCOM,我们的RFCOM比RLDM和RFRM都有明显的改进,可以用于重核裂变性质研究。发展了熔合-裂变过程的宏观模型,计算了形成复合核~(149)Tb、~(194)Hg的熔合过程及其相应的裂变过程。本工作对研究热核的形成及其衰变性无疑是很有用的

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重离子核反应机制的研究一直是人们关注的课题。入射能量较低时,集体效应占主要地位,反应为熔合反应及深部非弹性碰撞,实验可用平均场理论进行解释。当入射能量较高时,平均场效应消失,核子-核子碰撞起主要作用,实验可用参加者-旁观者模型来描述。中能区(10-100 MeV/u)的重离子反应既具有低能下一体耗散的特点,又具有高能下核子-核子碰撞的特征,由于作用时间短,非平衡现象变得很重要。在这一能区,多种反应机制共存并相互竞争。对这一能区的重离子核反应制的研究将有助于我们更清楚地了解原子核的结构。为此,我们在兰州重离子加速器HIRFL上进行了46.7 MeV/u ~(12)C引起的重离子反应中前方向出射产物的测量,着重讨论了周边反应中的弹核碎裂和转移反应以及它们的相互竞争。实验中用46.7 MeV/u ~(12)C束流轰击四种靶核:~(58)Ni、~(64)Ni、~(115)In和~(197)Au。通过对前方向出射的类弹碎片的测量,发现它们的平行动量分布宽度满足Goldhaber关系式,提取的约化平行动量分布宽度σ_0 = 80 ± 10 MeV/c,与相对论情形下的值接近,并且σ_0对于各种反应系统均相同。反应中弹核碎裂产物的最可几能量可用Abrasion图象来解释。对于质量接近弹核的类弹碎片,将碎裂部分和转移部分分开后,提取的转移部分的约化平行动量分布宽度为44 ± 10 MeV/c,这比弹核碎裂部分的宽度要窄,说明转移反应比弹核裂受到相空间中更严格的限制。弹核碎裂和转移反应的几率都随靶核质量增加而增加,并且与被转移结团的结构有关。转移反应主要对弹核附近的类弹碎片有贡献,当类弹碎片质量与弹核质量相差较大时,主要是弹核碎裂的贡献。对反应中的同位素产额分布也进行了分析,结果表明,类弹碎片的同位素分布对靶核有依赖关系,当靶核的N/Z增加时,产物的N/Z也增加,并且低能部分的N/Z比高能部分的N/Z要大。当角度变大时,~7Li/~6Li、~9Be/~7Be、~(11)B/~(10)B等同位素产额比随之变化,低能部分变化缓慢,高能部分则变化明显。产物的同位素产额分布或同位素产额比反映了系统由非平衡向平衡演化的过程。实验中对于BaF_2晶体与半导体组成的望远镜探测器的性能进行了测量。圆柱形BaF_2晶体后配以XP2020Q型光电倍增管,输出信号送入不同的QDC,以获得BaF_2中光输出的快慢成分。ΔE-E方法可以得到较好的元素鉴别,即使对低能的p、d、t也能分开,用快慢成分关联方法可对较高能量的轻带电粒子很好地鉴别。入射离子越重,相同能量的离子在BaF_2晶体中引起的光输出越小。BaF_2对入射离子的响应在较大的能区内是线性的,在低能时存在轻微的非线性。对80 cm大面积位置灵敏电离室与一维位置灵敏塑料闪烁体组成的探测系统首次在中能重离子反应中进行了测试。电离室可以测量较重的低能离子,有较好的粒子鉴别能力,能给出能量信息及两维位置信息。闪烁体则使得该系统可用于较高能量轻带电粒子的测量,它能给出能量吸一维位置信息,与电离室配合可以进行元素鉴别。它将在以后的中能重离子实验中得到广泛的应用

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In this article, a novel technique for the fabrication of surface enhanced Raman scattering (SERS) active silver clusters on glassy carbon (GC) has been proposed. It was found that silver clusters could be formed on a layer of positively charged poly(diallyldimethylammonium) (PDDA) anchored to a carbon surface by 4-aminobenzoic acid when a drop containing silver nanoparticles was deposited on it. The characteristics of the obtained silver clusters have been investigated by atomic force microscopy (AFM), SERS and an SERS-based Raman mapping technique in the form of line scanning. The AFM image shows that the silver clusters consist of several silver nanoparticles and the size of the clusters is in the range 80-100 nm. The SERS spectra of different concentrations of rhodamine 6G (R6G) on the silver clusters were obtained and compared with those from a silver colloid. The apparent enhancement factor (AEF) was estimated to be as large as 3.1 x 10(4) relative to silver colloid, which might have resulted from the presence of 'hot-spots' at the silver clusters, providing a highly localized electromagnetic field for the large enhancement of the SERS spectra of R6G. The minimum electromagnetic enhancement factor (EEF) is estimated to be 5.4 x 10(7) by comparison with the SERS spectra of R6G on the silver clusters and on the bare GC surface.

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A wet chemical approach is used successfully to produce nanostructured Au material by the reduction of sulfonated polyaniline (SPANI) nanotubes. The Au nanostructures obtained are composed of single crystal Au nanoplates, which are aggregated layer-by-layer into stacks or edge-on-face into clusters at various conditions. The Au nanoplate diameter and thickness can be conveniently controlled in the range of 100 nm to 2 mu m and 10 to 30 nm, respectively, with no accompanying single Au nanoparticles being observed. The formation of the Au nanostructures was controlled by the degradation of SPANI. The gradually and slowly released segments of SPANI served as the reductant during the growth of the 2D Au nanostructures.