104 resultados para rho-percolation


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Sb-doped and undoped ZnO thin films were deposited on Si (100) substrates by radio frequency (RF) magnetron sputtering. X-ray diffraction (XRD) and scanning electron microscopy (SEM) analyses revealed that all the films had polycrystalline wurtzite structure and c-axis preferred orientation. Room temperature Hall measurements showed that the as-grown films were n-type and conducting (rho similar to 1-10 Omega cm). Annealing in a nitrogen ambient at 400 degrees C for 1 h made both samples highly resistive (rho > 10(3) Omega cm). Increasing the annealing temperature up to 800 C, the resistivity of the ttndoped ZnO film decreased gradually, but it increased for the Sb-doped ZnO film. In the end, the Sb-doped ZnO film annealed at 800 C became semi-insulating with a resistivity of 10(4)Omega cm. In addition, the effects of annealing treatment and Sb-doping on the structural and electrical properties are discussed. (c) 2006 Elsevier B.V. All rights reserved.

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Magneto-transport measurements have been carried out on a Si heavily delta-doped In0.52Al0.48As/In(0.53)G(0.47)As single quantum well in the temperature range between 1.5 and 60 K under magnetic field up to 10 T. We studied the Shubnikov-de Haas(SdH) effect and the Hall effect for the In0.52Al0.48As/In(0.53)G(0.47)As single quantum well occupied by two subbands, and have obtained the electron concentration, mobility, effective mass and energy levels respectively. The electron concentrations of the two subbands derived from mobility spectrum combined with multi-carrier fitting analysis are well consistent with the result from the SdH oscillation. From fast Fourier transform analysis for d(2)rho/dB(2)-1/B, it is observed that there is a frequency of f(1)-f(2) insensitive to the temperature, besides the frequencies f(1), f(2) for the two subbands and the frequency doubling 2f(1), both dependent on the temperature. This is because That the electrons occupying the two different subbands almost have the same effective mass in the quantum well and the magneto-intersubband scattering between the two subbands is strong.

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We investigate theoretically the interplay between Zeeman splitting, Rashba spin-orbit interaction (RSOI), and Dresselhaus spin-orbit interaction (DSOI) and its influence on the magnetotransport property of two-dimensional electron gas (2DEG) at low temperature. Our theoretical results show that the nodes of the beating patterns of the magnetoresistivity rho(xx) for 2DEG with RSOI or DSOI alone depend sensitively on the total spin splitting induced by these three spin splitting mechanisms. It is interesting to find that the eigenstates in the presence of RSOI alone are connected with those in the presence of DSOI alone but with opposite Zeeman splitting by a time-reversal transformation. Consequently, the magnetoresistivities exhibit exactly the same oscillation patterns for these two cases. For strong RSOI or DSOI alone, the magneto-oscillation of rho(xx) shows two distinct periods. For 2DEG with both RSOI and DSOI, the beating patterns vanish for equal RSOI and DSOI strengths and vanishing Zeeman splitting. They will appear again, however, when Zeeman splitting or the difference between RSOI and DSOI strengths increases.

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Photoluminescence measurements have been performed in Si-rich a-SiNx:H (x less than or equal to 1.3) alloys prepared by glow discharge. It is observed that the blue shift of the peak of room temperature luminescence spectrum with increasing N content parallels increasing intensity. Two distinct luminescence mechanisms are proposed in a-SiNx:H with the threshold near x = 0.8. For low x, the samples show typical luminescence properties of a-Si:H, while for high x, the normalized luminescence bands are independent of temperature. Combining percolation theory, the luminescence origins are discussed on the basis of Brodsky's quantum well model. (C) 2000 Elsevier Science B.V. All rights reserved.

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The optical properties of Au nanoparticles deposited on thermochromic thin films of VO2 are investigated using spectroscopy. A localized modification on the transmittance spectrum of VO2 film is formed due to the presence of Au nanoparticles which exhibit localized surface plasmon resonance (LSPR) in the visible-near IR region. The position of the modification wavelength region shows a strong dependence on the Au mass thickness and shifts toward the red as it increases. On the other hand, it was found that the LSPR of Au nanoparticles can be thermally tunable because of the thermochromism of the supporting material of VO2. The LSPR wavelength, lambda(SPR), shifts to the blue with increasing temperature, and shifts back to the red as temperature decreases. A fine tuning is achieved when the temperature is increased in a stepwise manner.

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高分子凝胶广泛地存在于自然界以及日常生活中,按其形成作用力不同分为化学凝胶和物理凝胶两大类。由于高分子物理凝胶具有凝胶化的可逆性及其对环境条件强烈的响应性,因此,在近半个世纪的研究与应用中受到极大的关注。高分子溶液中的物理凝胶因其结构及形成机制复杂,在实验方面,除了散射技术及流变技术能够有效地揭示它的部分信息外,其它的实验手段很难用于这个领域的研究;在理论方面,化学凝胶的理论已经比较成熟,而物理凝胶的粘弹性质以及凝胶化是一个远离平衡态的松弛过程,除了一些特征的标度指数外,人们还没有得到适用于高分子物理凝胶的普适规律。当前,由于计算机模拟理论及模拟方法的发展,使得计算机模拟成为除了实验和理论研究方法之外的第三个重要的研究方法。但是,由于物理凝胶化行为的复杂性,用实验和理论获得的信息很难较好地描述凝胶化过程,而计算机模拟的高度透明性及反映信息的完整性,有助于理解这一复杂过程中所涉及的物理本质。因此,利用计算机模拟结合实验及理论方法深入研究高分子物理凝胶的形成机制、结构与性能关系已成为目前最有效的手段之一。 本论文主要运用Monte Carlo模拟方法,并结合小角中子散射(Small-Angle Neutron Scattering, SANS)和流变(Rheology)等实验手段从多个角度探讨了以下几类典型的高分子溶液物理凝胶化行为。 1. 温度对遥爪型三嵌段共聚物在选择性溶剂中的自组装及凝胶化行为影响的研究:采用二维简单方格子Monte Carlo模拟方法,结合逾渗(Percolation)理论,建立了溶胶-凝胶转变相图在统计热力学中的确定方法;甄别了具有特征构象的链,讨论了链及胶束的聚集,明晰了相互作用(体现为约化温度)、构象转变、聚集与凝胶化的一致的关联关系;提出了构象转变模型,进而明确了此体系的凝胶化过程,在微观尺度上表现为桥型链和环型链之间的竞争。 2. 模拟模型改进及其应用到持续长度对稀溶液中高分子链构象影响的研究:考虑到原始八位置键涨落模型效率低,实现复杂且不能应用到复杂的高分子体系,对该模型进行了改进,使其实现简单、效率高,并拓宽了该模型的应用范围。然后,以刚性对均聚物构象的影响为例,发现随着刚性增加,均聚物构象从球形椭球到棒状椭球的转变,并对比了自由连接链(Free Joint Chain, FJC)模型和蠕虫链(Wormlike Chain, WLC)模型在不同刚性范围内对高分子链末端距预测的偏差,首次给出了这两个经典模型的半定量的适用边界。 3. 溶剂尺寸对遥爪型三嵌段共聚物在选择性溶剂中的自组装及凝胶化行为影响的研究:用改进后的八位置键涨落Monte Carlo模型,研究了遥爪型三嵌段共聚物在选择性溶剂条件下的聚集和凝胶化对溶剂尺寸的依赖性,发现溶剂尺寸效应对凝胶化的作用是非单调的。由一个均聚物体系的对比模拟证明这种作用主要是由熵驱动的,并给出了中分子溶剂的半定量定义。在均聚物和嵌段共聚物溶液中,不同尺寸的溶剂分子可以使溶液由于高分子聚集不同而具有不同的微结构,并影响高分子链构象和溶液的性质。从多个角度研究了三嵌段共聚物在不同尺寸溶剂的溶液中所遵循的三种不同的凝胶化机理。 4. 聚氧化乙烯-氧化丙稀-氧化乙烯三嵌段共聚物(poly(ethylene oxide)-poly (propylene oxide)-poly-(ethylene oxide), PEO-PPO-PEO)重水溶液凝胶化的小角中子散射(SANS)和Monte Carlo研究:结合Pluronic F127(EO65PO99EO65)/D2O三嵌段共聚物溶液的特征,对照SANS数据,用改进后的八位置键涨落模型成功地从模拟中获得了F127/D2O的溶胶-凝胶转变相图。详细地考察了体系的微观结构,提出此类高分子溶液中形成的物理凝胶包含高分子逾渗网络的生成,以及被束缚溶剂(Bound Solvent)必须超过离散组分体系逾渗的临界体积分数的机理。着重研究了一定浓度的F127水溶液随温度升高引起的溶胶-凝胶转变以及凝胶-溶胶转变的Reentrant相行为,发现体系在低温区域的溶胶-凝胶转变遵循相同的机理,而在中等温度和较高温度以及不同浓度区域中的凝胶-溶胶转变遵循不同的机理。 5. 极性基团饱和度和溶剂条件对两亲性聚合物在溶液中的聚集行为和凝胶化影响的研究:用改进后的八位置键涨落模型,针对两亲性聚合物在不同溶剂条件的溶液建立了粗粒化模型,以两亲性聚合物中极性基团的饱和度,溶剂条件和高分子浓度为变量,考察了其对链构象、聚集及其凝胶化的影响。 6. 多糖水溶液凝胶化的流变和小角中子散射研究:用流变和SANS考察了两个多糖水溶液中物理凝胶化过程,针对由氢键主导的水基凝胶体系的典型特征进行了讨论,从分子链构象,聚集体结构及其关联以及流变特征等方面对聚强电解质角叉胶(Carrageenan)水溶液和聚弱电解质明胶(Pectin)水溶液进行了详细的讨论。考察了不同多糖的种类(聚合物链的电荷密度),盐的种类和浓度,溶液温度等对凝胶化和凝胶结构的影响,分析了不同多糖溶液的凝胶化机理。

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Ras 超家族蛋白是真核生物中普遍存在的一类小分子GTP 结合蛋白。它们 具有高度保守的GTP 结合结构域,根据序列结构和细胞功能被分为七个家族: Sar1、Arf、SRβ、Ran、Rab、Rho 和Ras。这些蛋白分别行使着真核生物特有的 细胞功能,诸如运输小泡的形成和转运(Sar1、Arf、Rab),胞质骨架的建成(Rho), 细胞核-胞质运输及核膜重建(Ran)等,其起源演化和真核细胞的起源密切相关。 本文利用生物信息学手段和分子生物学实验调查研究了原核生物和原生生物中 Ras 超家族蛋白同源物的存在情况,并进行了分子系统分析,对Ras 超家族蛋白 的起源演化问题进行了较为深入、系统的探讨。获得了以下结果和结论: 1)通过原核生物基因组的搜索和序列结构分析,在一些真细菌中首次鉴定 出了高度相似于真核生物Ras 超家族蛋白的原核生物同源物,且实验证明它们的 基因具有表达活性;在原细菌中的产甲烷菌和热原体中也发现有序列分歧较大的 同源物。并在更多的真细菌种类中鉴定出了更多的前人已报道的另一种小分子 GTP 结合蛋白—MglA。序列比对分析表明MglA 蛋白具有自己独特的序列特征, 与真核生物的Ras 超家族蛋白序列差异较大。进一步的分子系统分析显示:真核 生物Ras 超家族蛋白的七个家族中,Ran、Rab、Rho 和Ras 等四个家族聚在一 起,上述我们所鉴定的真细菌的Ras 超家族蛋白同源物则紧聚在其外围;真核生 物的另三个家族(Sar1、Arf、SRβ)聚成另一枝,并接着与产甲烷原细菌的的同 源物及真细菌的MglA 蛋白聚在一起。这些结果表明:Ras 超家族蛋白不是前人 所认为的为真核生物所特有,实际上在一些原核生物中就已产生;真核生物Ras 超家族蛋白的祖先也不太可能是前人所认为的为真细菌的MglA;真核生物Ras 超家族蛋白的七个家族可能有两种不同的起源:Ran、Rab、Rho 和Ras 等可能 来源于蓝细菌或蛋白菌,或二者的共同祖先,而Sar1、Arf 和SRβ 可能来源于产 甲烷原细菌,这也可能反映了真核细胞“融合起源”的历史。 2)通过搜索一些较为低等的单细胞真核生物——原生生物基因组中Ras 超 家族蛋白,并结合一系列其他处在不同进化地位真核生物的Ras 超家族蛋白进行 分析,发现Sar1、Arf、Rab 和Ran 家族的蛋白在真核生物中普遍存在,而SRβ、 Rho 和Ras 家族蛋白在有些真核生物中未找到。根据各家族蛋白在真核生物中的分布情况推测在真核生物的最近共同祖先中存在的Ras 超家族蛋白可能有下列 两种情况:(1)最近的共同祖先已经具有了所有七个家族的蛋白,并且至少有 11 个成员:1 个Sar1、1 个SRβ、3 个Arf(Arf1、Arl1、Arl2)、3 个Rab(Rab1、 Rab6、Rab11)、1 个Ran、1 个Rho(Rac)和1 个Ras(RheB)。因而,部分真 核生物中缺少SRβ、Rho 和Ras 家族蛋白很可能是因基因丢失所致。植物中Ras 家族蛋白的缺少应该是由于在进化早期,其祖先绿藻丢失了单个Ras 家族蛋白基 因所致;(2)根据Cavalier-Smith 的真核生物划分为单鞭毛(变形虫类、真菌和 后生动物)和双鞭毛(藻类、植物和除变形虫外的原生动物)两大类的分类观点, 真核生物最近的共同祖先可能只具有除Ras 家族而外的六个家族的成员,而Ras 家族蛋白则是在此两大类群分化以后在单鞭毛类生物中才产生的,多数双鞭毛类 生物如原生动物、绿藻和植物中没有Ras 的情况应该是一种祖征,而个别双鞭毛 类生物如红藻具有的Ras 家族蛋白则很可能是从单鞭毛类生物那里水平基因转 移而来的。至于SRβ 和Rho 家族蛋白在部分物种中的缺少,则还是可能因为基 因丢失所致。此外,变形虫类生物中大量的Ras 超家族蛋白提示基因组的大小或 进化地位的高低并不是Ras 超家族蛋白成员多少的决定性因素,而细胞相应生理 活动的需求才是家族成员增多的关键。

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Electrical, structural and reaction characteristics of In-based ohmic contacts to n-GaAs were studied. Attempts were made to form a low-band-gap interfacial phase of InGaAs to reduce the barrier height at the metal/semiconductor junction, thus yielding low-resistance, highly reliable contacts. The contacts were fabricated by e-beam sputtering Ni, NiIn and Ge targets on VPE-grown n(+)-GaAs film (approximate to 1 mu m, 2 x 10(18) cm(-3)) in ultrahigh vacuum as the structure of Ni(200 Angstrom)/NiIn(100 Angstrom)/Ge(40 Angstrom)/n(+)-GaAs/SI-GaAs, followed by rapid thermal annealing at various temperatures (500-900 degrees C). In this structure, a very thin layer of Ge was employed to play the role of heavily doping donors and diffusion limiters between In and the GaAs substrate. Indium was deposited by sputtering NiIn alloy instead of pure In in order to ensure In atoms to be distributed uniformly in the substrate; nickel was chosen to consume the excess indium and form a high-temperature alloy of Ni3In. The lowest specific contact resistivity (rho(c)) of (1.5 +/- 0.5)x 10(-6) cm(2) measured by the Transmission Line Method (TLM) was obtained after annealing at 700 degrees C for 10 s. Auger sputtering depth profile and Transmission Electron Microscopy (TEM) were used to analyze the interfacial microstructure. By correlating the interfacial microstructure to the electronical properties, InxGa1-xAs phases with a large fractional area grown epitaxially on GaAs were found to be essential for reduction of the contact resistance.

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本研究针对北方地区的实际情况,依据水量平衡原理,采取田间试验方法,通过蒸散试验、测筒试验、阻渗试验和无阻渗条件下灌水试验,研究了3种灌水处理(淹灌、湿润灌和间歇灌)条件下水稻蒸腾、稻田棵间蒸发和稻田蒸散的变化规律,以及3种阻渗处理(薄膜阻渗、厚膜阻渗和土壤夯实阻渗)条件下稻田的阻渗效果及无阻渗条件下2种灌水处理(淹灌和间歇灌)对稻田渗漏的影响。研究结果表明:1、湿润灌处理的蒸散量与其它两种灌水处理的蒸散量具有显著差别,3种灌水处理的产量差别不显著,与淹灌相比,湿润灌处理的水分利用效率可以提高23.9~31.2%;2、3种灌水处理的水稻蒸腾量没有显著差别;3、3种灌水处理条件下的稻田棵间蒸发量,以湿润灌最小,与淹灌和间歇灌相比,分别减少38.8和26.6%的蒸发量;4、0.007mm厚的薄膜阻渗效果不明显;0.03mnl厚的厚膜处理和土壤夯实处理具有明显的阻渗效果,与对照(无阻渗)相比,可以减少23.7~47.3%渗漏量;5、无阻渗条件下,与淹灌处理相比,间歇灌水处理的渗漏量,在整个稻作生产期(包括泡田期和水稻整个生育期)内减少15.2%;6、不同阻渗处理和无阻渗条件下2种灌水处理之间的产量无显著差别,以厚膜阻渗处理和夯实处理的水分利用效率最高,无阻渗条件下淹灌处理的水分利用效率最低。

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The motion of a single bubble rising freely in quiescent non-Newtonian viscous fluids was investigated experimentally and computationally. The non-Newtonian effects in the flow of viscous inelastic fluids are modeled by the Carreau theological model. An improved level set approach for computing the incompressible two-phase flow with deformable free interface is used. The control volume formulation with the SIMPLEC algorithm incorporated is used to solve the governing equations on a staggered Eulerian grid. The simulation results demonstrate that the algorithm is robust for shear-thinning liquids with large density (rho(1)/rho(g) up to 10(3)) and high viscosity (eta(1)/eta(g) up to 10(4)). The comparison of the experimental measurements of terminal bubble shape and velocity with the computational results is satisfactory. It is shown that the local change in viscosity around a bubble greatly depends on the bubble shape and the zero-shear viscosity of non-Newtonian shear-thinning liquids. The shear-rate distribution and velocity fields are used to elucidate the formation of a region of large viscosity at the rear of a bubble as a result of the rather stagnant flow behind the bubble. The numerical results provide the basis for further investigations, such as the numerical simulation of viscoelastic fluids. (C) 2010 Elsevier B.V. All rights reserved.

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Within an isospin- and momentum-dependent hadronic transport model, it is shown that the recent FOPI data on the pi(-)/pi(+) ratio in central heavy-ion collisions at SIS/GSI energies [Willy Reisdorf , Nucl. Phys. A 781, 459 (2007)] provide circumstantial evidence suggesting a rather soft nuclear symmetry energy E-sym(rho) at rho >= 2 rho(0) compared to the Akmal-Pandharipande-Ravenhall prediction. Some astrophysical implications and the need for further experimental confirmations are discussed.

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We report some recent progress in constraining the symmetry energy E-sym(rho) at high densities using high-energy heavy-ion collisions. Circumstantial evidence of a soft E-sym(rho) at supra-saturation density is obtained by comparing the pion ratio pi(-)/pi(+) measured recently with FOPI at GSI and the IBUU04 model calculations. Detailed studies indicate that the power of determining the E-sym(rho)from pi(-)/pi(+) is enhanced with decreasing the beam energy to near the pion production threshold, showing a correlation to the increasing nuclear stopping. Among several heavy-ion reaction facilities in the world, the cooling storage ring (HIRFL-CSR), newly commissioned at Lanzhou, delivering heavy-ion beams up to 1 A GeV, to be coupled with advanced detectors will contribute significantly to further studies of the equation of state of asymmetric nuclear matter.

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The multi-configuration Dirac Fock (MCDF) method is implemented to study doubly excited 2s2p P-1,3(1) resonances of the helium atom and the interference between photoionization and photo excitation autoionization processes. In order to reproduce the total photoionization sprectra, the excited energies from the ground 1s(2) S-1(0) state to the doubly excited 2s2p P-1,3(1) states and the relevant Auger decay rates and widths are calculated in detail. Further more, the interference profile determined by the so-called Fano parameters q and rho(2) is also reproduced. Good agreement is found between the present results and other available theoretical and experimental results. This indeed shows a promising way to investigate the Fano resonances in photoionization of atoms within the MCDF scheme, although there are some discrepancies in the present calculations of the 2s2p P-3(1) state.

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The reactions pi(-)p -> eta n and gamma p -> eta p are investigated within a dynamical coupled-channels model of meson production reactions in the nucleon resonance region The meson-baryon channels included are pi N, pi Delta, sigma N, and rho N The direct eta-photoproduction process is studied within a formalism based on a chiral constituent quark model approach, complemented with a one-gluon-exchange mechanism, to take into account the breakdown of the SU(6)circle times O(3) symmetry In the models search, the following known nucleon resonances are embodied S-11(1535), S-11(1650), P-11(1440), P-11(1710), P-13(1720), D-13(1520), D-13(1700), D-15(1675), and F-15(1680). Data for the pi(-)p -> eta n reaction from threshold up to a total center-of-mass energy of W approximate to 2 GeV are satisfactorily reproduced For the photoproduction channel: two additional higher mass known resonances, P-13(1900) and F-15(2000), are also considered However, reproducing the data for gamma p -> eta p requires, within our approach, two new nucleon resonances, for which we extract, mass and width

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Hard photons from neutron-proton bremsstrahlung in intermediate energy heavy-ion reactions are examined as a potential probe of the nuclear symmetry energy within a transport model. Effects of the symmetry energy on the yields and spectra of hard photons are found to be generally smaller than those due to the currently existing uncertainties of both the in-medium nucleon-nucleon cross sections and the photon production probability in the elementary process pn -> pn gamma. Very interestingly, nevertheless, the ratio of hard photon spectra R-1/2(gamma) from two reactions using isotopes of the same element is not only approximately independent of these uncertainties but also quite sensitive to the symmetry energy. For the head-on reactions of Sn-132 + Sn-124 and Sn-112 + Sn-112 at E-beam/A = 50 MeV, for example, the R-1/2(gamma) displays a rise up to 15% when the symmetry energy is reduced by about 20% at rho = 1.3 rho(0) which is the maximum density reached in these reactions. (C) 2008 Elsevier B.V. All rights reserved.