24 resultados para Strong potential models

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本文以中国科学院成都生物研究所培育的同源四倍体水稻和二倍体水稻为材料,进行遗传差异及产量、品质性状的研究:1、以二倍体水稻为对照,研究了同源四倍体水稻在2004 年和2005 年的结实情况。结果同源四倍体的花粉育性、结实率均不同程度下降,尤其低代材料更是大幅度下降。F 检验表明,同源四倍体不同个体间的各产量性状均差异显著,说明其具有很大的遗传改良潜力。从1996 年到2005 年对部分同源四倍体水稻进行了连续选择改良,T 检验表明经过9 年的选择改良,其结实率显著提高。本文还对同源四倍体水稻各产量性状间的相关性进行了分析,结果结实率与花粉育性、穗着粒数、穗实粒数极显著相关;理论产量与花粉育性、有效穗数、穗着粒数、穗实粒数、结实率及千粒重极显著相关。i2、用(CT)n 微卫星标记和PCR-Acc Ι分子标记对40 份同源四倍体和14 份二倍体水稻Wx 基因进行研究。结果,(CT)n 微卫星标记检测,Wx 基因呈Wx1、Wx2 和Wx3 3 种多态性;PCR-Acc Ι 检测,Wx 基因表现为G-型和T-型。测定稻米直链淀粉含量(AC)、胶稠度(GC)和糊化温度(GT),并探讨其与Wx 基因的关系,结果,二倍体和同源四倍体水稻均存在:Wx 基因型相同,AC 差异较小,Wx 基因型不同时,AC 差异较大,Wx1 基因型品种AC 最高, Wx2 基因型品种AC 次之,Wx3 基因型品种AC 最低;基因型相同时,同源四倍体AC 低于二倍体;同源四倍体与对应二倍体间,Wx 基因型相同时,AC 差异很小;而Wx 基因型发生变异时,AC 差异很大。同时,进行相关性分析,结果二倍体和四倍体水稻均存在AC、GC 与Wx 基因密切相关;而GT 与Wx 基因相关不显著。综合分析,(CT)n微卫星标记与PCR-Acc Ι 分子标记检测的相关系数为0.842,呈极显著正相关,可以将其结合起来进行同源四倍体新品种的选育和改良。3、利用RAPD 技术,对同源四倍体和二倍体水稻的遗传差异进行分析。17条引物在同源四倍体中扩增出178 条带(PPB=81.5%),在二倍体中扩增出173条带(PPB=76.3%);同源四倍体和二倍体的Shannon 遗传多样性指数分别为0.4848 和0.4679,多态信息量分别为0.3301 和0.3216,遗传距离分别为0.3572和0.3460;同源四倍体与其对应二倍体间遗传距离为0.1914-0.4633,平均为0.2914。表明同源四倍体的遗传多样性高于二倍体,且同源四倍体与其二倍体之间存在较大的遗传差异,这些将为水稻品种改良和新品种选育提供科学依据。上述产量、品质性状及遗传差异分析的结果,不仅有利于加快同源四倍体水稻的遗传改良进程,而且为进一步研究、利用同源四倍体水稻奠定了初步基础。 AbstractStudy on genetic diversity, yield characters and quality traitsof autotetraploid and diploid riceLiu Yuhua (Botany)Directed by Associate Prof. Tu ShengbinIn this study, diploid and autotetraploid rice, which were cultivated in ChengduInstitute of Biology were analyzed in genetic diversity, yield characters and qualitytraits.In the study, 2 diploid and 29 autotetraploid rice(2n=4x=48) materials, including4 preliminary and 25 advanced generation, were investigated for yield characters.Compared with diploid check, the pollen fertility and seed set of autotetraploiddeclined dramatically, especially in preliminary generation. F-test indicated that therewere remarkable differences among different varieties, showing that autotetraploidmaterials had strong potential for improvement. From 1996 to 2005, someautotetraploid rice had been selected and improved. T-test showed that seed setincreased obviously. The relationships among yield characters of autotetraploid ricewere analyzed. Seed set was strongly correlated with pollen fertility, total grainnumber per panicle and productive grain number per panicle; theoretical yield wasstrongly correlated with pollen fertility, productive panicle number per plant, totalgrain number per panicle, productive grain number, seed set and 1000-grain weight.Wx genotypes of 40 autotetraploid rice and 14 diploid rice were tested by usingthe (CT)n microsatellite marker and a cleaved amplified polymorphic sequence(CAPS) molecular marker named PCR-Acc Ι. Three microsatellite alleles wereproduced, i.e. Wx1, Wx2 and Wx3 both in autotetraploid and in diploid rice.Comparatively, PCR- Acc Ι molecular marker produced two genotypes, G-type andT-type for both autotetraploid and diploid rice. In this study, amylose content (AC), gel of consistency (GC) and gelatinization temperature (GT) of rice grain weremeasured and their relationships with Wx alleles were analyzed. The results showedthat variation of AC between autotetraploid and diploid rice was small when they hadthe same Wx genotype. However, variation of AC turned to be large when the Wxgenotypes were different. Actually, AC met the maximum value in Wx1 varieties andWx2 varieties the middle and Wx3 varieties the minimum. And AC was lower inautotetraploid than in diploid. Correlation analysis was done in this experiment. ACand GC of rice grain were probably controlled by Wx gene or other gene whoselocation was strictly linked to Wx gene, while GT of rice was not. The correlationcoefficient between Wx genotypes which revealed by (CT)n microsatellite marker andPCR-Acc Ι molecular marker was 0.842 with significant level. That revealed aconsistent result between the two types of markers. So it was possible to utilize boththe two types of markers to select and promote germplasm of autotetraploid rice.RAPD molecular markers were used to analyze the genetic diversity betweendiploid and autotetraploid rice. 178 repeatable bands were detected through 17 RAPDprimers with percentage of polymorphic bands was 81.5% in autotetraploid rice while173 repeatable bands were detected with percentage of polymorphic bands was 76.3%in diploid rice. According to the measurement of Shannon index, polymorphicinformation content and genetic distance, genetic diversity of autotetraploid was on ahigher level, genetic variation between autotetraploid and diploid rice was relativelyhigh. All these contributed to the genetic selection and improvement in rice breeding.As mentioned above, the results are not only helpful to promote the process ofrice improvement, but also to confirm the basic for further study of autotetraploid rice.

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人类的载脂蛋白A5(apolipoprotein A5,APOA5)是一个新近发现的载脂蛋白家族成员。它在血浆中的含量比其他载脂蛋白低1-2个数量级,但能显著影响血浆三酰甘油水平,对血脂代谢具有重要意义,可以作为降血脂药物治疗中一个强有力的潜在靶标。 由于APOA5在血浆中含量低,直接从血浆中分离纯化很困难,国内一直没有报道简易可靠的纯化方法。为进一步研究APOA5的生物学特性,探讨其与TG代谢中的其它关键成分之间的相互关系,揭示其在脂类代谢相关疾病中的重要地位,必须有大量的蛋白和抗体用于基础研究。因此本研究首先利用基因工程技术,诱导表达纯化APOA5蛋白,免疫动物制备多克隆抗体,为进一步研究人肝脏细胞中APOA5的相互作用蛋白,研究APOA5蛋白在肝脏细胞中的功能奠定基础。 为了深入研究APOA5在肝脏中如何行使功能,我们采用细菌双杂交技术寻找与APOA5相互作用的蛋白因子。并采用Pull-down技术,免疫荧光及免疫共沉淀技术进一步确证其在体外和体内的相互作用关系,为进一步阐明APOA5在体内的生理功能提供了新的线索。 第一部分 APOA5基因的克隆、原核表达、纯化及其多克隆抗体的制备 本研究首先应用基因克隆技术,从人肝癌细胞系SMMC-7721的cDNA中扩增出1.1 kb的ApoA5基因全长序列。然后将其克隆至表达载体pThioHisD,构建原核表达载体pTH-APOA5。该重组质粒转化至大肠杆菌 BL21(DE3),成功实现人APOA5融合蛋白在大肠杆菌中的表达。经发酵得到高效表达的融合蛋白。 融合蛋白在 IPGT 诱导下以包涵体的形式大量表达。利用融合蛋白上的一段组氨酸序列,用镍离子亲和柱进行纯化和复性后,获得较高纯度的人APOA5融合蛋白。利用该融合蛋白免疫新西兰大耳白兔,获得了高效价的兔抗人APOA5多克隆抗体,Western Blot结果显示此多克隆抗体与APOA5特异性结合。 第二部分 细菌双杂交筛选与APOA5相互作用的蛋白 本实验首先构建了pBT-APOA5重组质粒,经双酶切、PCR和测序鉴定证明重组诱饵质粒构建成功,并进行了表达、自激活鉴定。Western Blot鉴定证实报告菌株中表达了分子量为 68 kD左右的重组融合蛋白,与预测的分子量APOA5(41 kD)/lamda cI (27 kD)一致。自激活实验证明诱饵蛋白不能单独激活报告基因,可用于筛选人肝脏cDNA文库。经过双重抗性筛选和回复筛选,分离出10个阳性克隆。对结果进行生物信息学分析,得到7个与APOA5相互作用的蛋白,其中BI1为细胞凋亡调节因子;ATP6、CYTB、ND2、COX-1为线粒体表达蛋白; ALB、TTR为血清蛋白。 第三部分 APOA5与BI1相互作用的确证 首先构建了BI1的原核表达载体pGEX-5X-3-BI1,利用Pull-down实验检测了APOA5与BI1在体外具有相互作用。然后构建了BI1的真核表达载体pCDNA3.1-HA-BI1和APOA5的真核表达载体pCDNA3.1-APOA5,并验证其表达。通过免疫荧光细胞内共定位研究发现,靶蛋白APOA5主要分布于胞浆,与BI1在HEK293细胞有共定位,即APOA5与BI1存在相互作用的可能。最后利用免疫共沉淀手段,在HEK293细胞中确证了靶蛋白APOA5与BI1在体内的相互作用。 上述研究结果,为深入研究APOA5在体内的生物学功能提供了新的思路。 Apolipoprotein A5 (APOA5) is a newly discovered protein belongs to apolipoprotein family. APOA5’s concentration is 1-2 orders of magnitude lower than other apolipoproteins in the circulation. APOA5 significantly affected plasma triglyceride levels, which is important on lipid metabolism. APOA5 has strong potential to be used as a hypolipidemic drug target. Large amount of APOA5 protein and antibodies are needed in basic research, such as biological characteristics study of the APOA5, its relationship with other key components in TG metabolism, its role played in Lipid metabolism-related diseases. Due to its low concentration in plasma, separation and purification of APOA5 from the plasma is very difficult. Until now no report on simple and reliable method for purification has been published in China. In this study, we firstly got APOA5 recombinant protein using genetic engineering technology. The purified recombinant protein was used to immunize rabbits to get antiserum. It is important for further study of the APOA5 protein-interacting protein. And it lays the foundation for studing APOA5 function in liver. In order to study APOA5 function in liver, we used bacterial two-hybrid technology to find the APOA5 protein interactor. Pull-down, immunofluorescence and immunoprecipitation techniques were used to further confirm the interaction between APOA5 with its interactor in vitro and in vivo. All of these stdudies provided new clues on its physiological functions in vivo. Part I: Cloning, prokaryotic expression, purification and polyclonal antibody preparation of APOA5 First of all, we amplified APOA5 CDS sequence from the human hepatoma cell line SMMC-7721, and subcloned into Expression vector pThioHisD, and got the recombinants named pTH-APOA5. The plasmid was transformed to BL21 (DE3). E. coli BL21(DE3) cells bearing the pTH-APOA5 plasmid were cultured and APOA5 protein synthesis was induced by the addition of IPTG. Recombinant protein was expression in the form of inclusion. Inclusion bodies were dissolved in phosphate-buffered saline containing 8 M urea and 40 mM imidazole, then applied to a Ni2+ affinity column, and were eluted in a buffer containing 4 M urea and 200 mM imidazole. Fractions containing the APOA5 protein were pooled and dialyzed against buffer containing phosphate-buffered saline. Antiserum to recombinant human APOA5 was generated by immuning rabbit. Western Blot showed that this antiserum specific binding with APOA5. Part II Two-hybrid system screening protein interactions with the APOA5 The coding sequence of human APOA5 was amplified using synthetic oligonucleotide primers from pTH-APOA5 vector and was subcloned into the pBT plasmidc to yield pBT-APOA5 vector. DNA sequencing was performed to verify that no unwanted mutations occurred during the process of plasmid vector construction. We verified recombinant protein expression and tested self-activation by pBT-APOA5 prior to screening. Western Blot verified inducing a 68 kD band, consistent with the predicted molecular weight (APOA5 41 kD, lamda cI 27 kD). pBT-APOA5 can be used for screening human liver cDNA library because it can not self-activation. Totally 10 positive clones were isolated. The nucleotide sequence of the positive clones were determined and compared to NCBI nucleotide sequence databases. We got 7 protein which interact with APOA5, included BI1(Apoptosis regulator); ATP6, CYTB, ND2, COX-1(Mitochondrial protein) and ALB, TTR(Serum protein). Part III Confirming of interaction between APOA5 with BI1 pGEX-5X-3-BI1 vector was subcloned at first. Pull-down experiments were used to detect the interaction between APOA5 with BI1 in vitro. Later, pCDNA3.1-HA-BI1 and pCDNA3.1-APOA5 were subcloned. Through immunofluorescence co-localization study, we found APOA5 mainly distributed in the cytoplasm. APOA5 is co-localization with BI1 in HEK293 cells. Finally, we verified interaction between APOA5 with BI1 in vivo through immunoprecipitation.

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Geological fluids are important components in the earth system. To study thephysical chemistry properties and the evolution of fluid system turns out to be one of the most challenging issues in geosciences. Besides the conventional experimental approaches and theoretical or semi-theoretical modeling, molecular level computer simulation(MLCS) emerges as an alternative tool to quantificationally study the physico-chemical properties of fluid under extreme conditions in order to find out the characteristics and interaction of geological fluids in and around earth. Based on our previous study of the intermolecular potential for pure H2O and thestrict evaluation of the competitive potential models for pure CH4 and the ab initio fitting potential surface across H2O-CH4 molecules in this study, we carried out more than two thousand molecular dynamics simulations for the PVTx properties of pure CH4 and the H2O-CH4 mixtures. Comparison of 1941 simulations with experimental PVT data for pure CH4 shows an average deviation of 0.96% and a maximum deviation of 2.82%. The comparison of the results of 519 simulations of the mixtures with the experimental measurements reveals that the PVTx properties of the H2O-CH4 mixtures generally agree with the extensive experimental data with an average deviation of 0.83% and 4% in maximum, which is equivalent to the experimental uncertainty. Moreover, the maximum deviation between the experimental data and the simulation results decreases to about 2% as temperature and pressure increase,indicating that the high accuracy of the simulation is well retained in the high temperature and pressure region. After the validation of the simulation method and the intermolecular potential models, we systematically simulated the PVTx properties of this binary system from 673 K and 0.05 GPa to 2573 K and 10 GPa. In order to integrate all the simulation results and the experimental data for the calculation of thermodynamic properties, an equation of state (EOS) is developed for the H2O-CH4 system covering 673 to 2573 K and 0.01 to 10 GPa. Isochores for compositions < 4 mol% CH4 up to 773 K and 600 MPa are also determined in this thesis.

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Qubit measurement by mesoscopic charge detectors has received great interest in the community of mesoscopic transport and solid-state quantum computation, and some controversial issues still remain unresolved. In this work, we revisit the continuous weak measurement of a solid-state qubit by single electron transistors (SETs) in nonlinear-response regime. For two SET models typically used in the literature, we find that the signal-to-noise ratio can violate the universal upper bound "4," which is imposed quantum mechanically on linear-response detectors. This different result can be understood by means of the cross correlation of the detector currents by viewing the two junctions of the single SET as two detectors. Possible limitation of the potential-scattering approach to this result is also discussed.

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A new interface anisotropic potential, which is proportional to the lattice mismatch of interfaces and has no fitting parameter, has been deduced for (001) zinc-blende semiconductor interfaces. The comparison with other interface models is given for GaAs/AlAs and GaAs/InAs interfaces. The strong influence of the interface anisotropic potential on the inplane optical anisotropy of GaAs/AlGaAs low dimensional structures is demonstrated theoretically within the envelope function approximation.

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Maps of surface chlorophyllous pigment (Chl a + Pheo a) are currently produced from ocean color sensors. Transforming such maps into maps of primary production can be reliably done only by using light-production models in conjuction with additional information about the column-integrated pigment content and its vertical distribution. As a preliminary effort in this direction. $\ticksim 4,000$ vertical profiles pigment (Chl a + Pheo a) determined only in oceanic Case 1 waters have been statistically analyzed. They were scaled according to dimensionless depths (actual depth divided by the depth of the euphotic layer, $Z_e$) and expressed as dimensionless concentrations (actual concentration divided by the mean concentration within the euphotic layer). The depth $Z_e$ generally unknown, was computed with a previously develop bio-optical model. Highly sifnificant relationships were found allowing $\langle C \rangle_tot$, the pigment content of the euphotic layer, to be inferred from the surface concentration, $\bar C_pd$, observed within the layer of one penetration depth. According to their $\bar C_pd$ values (ranging from $0.01 to > 10 mg m^-3$), we categorized the profiles into seven trophic situations and computed a mean vertical profile for each. Between a quasi-uniform profile in eutrophic waters and a profile with a strong deep maximum in oligotrophic waters, the shape evolves rather regularly. The wellmixed cold waters, essentially in the Antarctic zone, have been separately examined. On average, their profiles are featureless, without deep maxima, whatever their trophic state. Averaged values their profiles are featureless, without deep maxima, whatever their trophic state. Averaged values their profiles are featureless, without deep maxima, whatever their trophic state. Averaged values of $ρ$, the ratio of Chl a tp (Chl a + Pheo a), have also been obtained for each trophic category. The energy stored by photosynthesizing algae, once normalized with respect to the integrated chlorophyll biomass $\langle C \rangle _tot $ is proportional to the available photosythetic energy at the surface via a parameter $ψ∗$ which is the cross-section for photosynthesis per unit of areal chlorophyll. By tanking advantage of the relative stability of $ψ∗.$ we can compute primary production from ocean color data acquired from space. For such a computation, inputs are the irradiance field at the ocean surface, the "surface" pigment from which $\langle C \rangle _tot$ can be derived, the mean $ρ value pertinent to the trophic situation as depicted by the $\bar C_pd or $\langle C \rangle _tot$ values, and the cross-section $ψ∗$. Instead of a contant $ψ∗.$ value, the mean profiles can be used; they allow the climatological field of the $ψ∗.$ parameter to be adjusted through the parallel use of a spectral light-production model.

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A general formulation of the Helmholtz free energy used in thermodynamics of damage process of rocks is derived within a multi-scale framework. Such a physically-based thermodynamic state potential has a hybrid, discrete/continuum, nature in the sense tha

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Two types of peeling experiments are performed in the present research. One is for the Al film/Al2O3 substrate system with an adhesive layer between the film and the substrate. The other one is for the Cu film/Al2O3 substrate system without adhesive layer between the film and the substrate, and the Cu films are electroplated onto the Al2O3 substrates. For the case with adhesive layer, two kinds of adhesives are selected, which are all the mixtures of epoxy and polyimide with mass ratios 1:1.5 and 1:1, respectively. The relationships between energy release rate, the film thickness and the adhesive layer thickness are measured during the steady-state peeling process. The effects of the adhesive layer on the energy release rate are analyzed. Using the experimental results, several analytical criteria for the steady-state peeling based on the bending model and on the two-dimensional finite element analysis model are critically assessed. Through assessment of analytical models, we find that the cohesive zone criterion based on the beam bend model is suitable for a weak interface strength case and it describes a macroscale fracture process zone case, while the two-dimensional finite element model is effective to both the strong interface and weak interface, and it describes a small-scale fracture process zone case. (C) 2007 Elsevier Ltd. All rights reserved.

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Based on the introduction of the traditional mathematical models of neurons in general-purpose neurocomputer, a novel all-purpose mathematical model-Double synaptic weight neuron (DSWN) is presented, which can simulate all kinds of neuron architectures, including Radial-Basis-Function (RBF) and Back-propagation (BP) models, etc. At the same time, this new model is realized using hardware and implemented in the new CASSANN-II neurocomputer that can be used to form various types of neural networks with multiple mathematical models of neurons. In this paper, the flexibility of the new model has also been described in constructing neural networks and based on the theory of Biomimetic pattern recognition (BPR) and high-dimensional space covering, a recognition system of omni directionally oriented rigid objects on the horizontal surface and a face recognition system had been implemented on CASSANN-H neurocomputer. The result showed DSWN neural network has great potential in pattern recognition.

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A prominent effect of the interface potential (IP) [E. L. Ivchenko and A. Yu. Kaminski, Phys. Rev. B 54, 5852 (1996); O. Krebs and P. Voisin, Phys. Rev. Lett. 77, 1829 (1996)], the optical anisotropy of the forbidden transitions in quantum wells has been observed by reflectance-difference spectroscopy. Predictions by the heavy-light-hole coupling IP models are qualitatively consistent with all the observed features of the forbidden and the allowed transitions. The fact that the predicted value of the relative, transition strength, which depends on neither the IP strength nor the electric field, disagrees with the observed one indicates that coupling involving X and/or L bands may also be important. [S0163-1829(99)04227-7].

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By using three analytical phonon models in quantum wells-the slab model, the guided-mode model, and the improved version of the Huang-Zhu model [Phys. Rev. B 38, 13 377 (1998)], -and the phonon modes in bulk, the energy-loss rates of hot carriers due to the Frohlich potential scattering in GaAs/AlAs multiple quantum wells (MQW's) are calculated and compared to those obtained based on a microscopic dipole superlattice model. In the study, a special emphasis is put on the effects of the phonon models on the hot-carrier relaxation process when taking the hot-phonon effect into account. Our numerical results show that, the calculated energy-loss rates based on the slab model and on the improved Huang-Zhu model are almost the same when ignoring the hot-phonon effect; however, with the hot phonon effect considered, the calculated cooling rate as well as the hot phonon occupation number do depend upon the phonon models to be adopted. Out of the four analytical phonon models investigated, the improved Huang-Zhu model gives the results most close to the microscopic calculation, while the guided-mode model presents the poorest results. For hot electrons with a sheet density around 10(12)/cm(2), the slab model has been found to overestimate the hot-phonon effect by more than 40% compared to the Huang-Zhu model, and about 75% compared to the microscopic calculation in which the phonon dispersion is fully included. Our calculation also indicates that Nash's improved version [J. Lumin. 44, 315 (1989)] is necessary for evaluating the energy-loss rates in quantum wells of wider well width, because Huang-Zhu's original analytical formulas an only approximately orthogonal for optical phonons associated with small in-plane wave numbers. [S0163-1829(99)08919-5].

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InN films with electron concentration ranging from n similar to 10(17) to 10(20) cm(-3) grown by metal-organic chemical vapor deposition (MOCVD) and molecular beam epitaxy (MBE) were investigated by variable-temperature photoluminescence and absorption measurements. The energy positions of absorption edge as well as photoluminescence peak of these InN samples with electron concentration above 10(18) cm(-3) show a distinct S-shape temperature dependence. With a model of potential fluctuations caused by electron-impurity interactions, the behavior can be quantitatively explained in terms of exciton freeze-out in local potential minima at sufficiently low temperatures, followed by thermal redistribution of the localized excitons when the band gap shrinks with increasing temperature. The exciton localization energy sigma (loc) is found to follow the n (5/12) power relation, which testifies to the observed strong localization effects in InN with high electron concentrations.

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A theoretical investigation of ballistic electron transport in a quantum wire with soft wall confinement is presented. A general method of the electron transmission calculation is proposed for structures with complicated geometries. The effects of the lateral guiding potential on ballistic transport are investigated using three soft wall confinement models and the results are compared with those obtained from the hard wall confinement approximation. It is shown that the calculated transmission coefficients are notably dependent on the lateral confining potential especially when the incident electron energy is larger than the energy of the second transverse mode. It is found that the transmission profile obtained from soft wall confinement models exhibits simpler resonance structures than that obtained from the hard wall confinement approximation. Our results suggest that only in the single-channel regime the hard wall confinement approximation can give reasonable results.

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In this paper, we study the ability of DNA-PK-deficient (M059J) and -proficient (M059K) cells to undergo the rate of cellular proliferation, cell cycle distribution and apoptosis after 10 Gy X-ray irradiation, and the role of DNA-PK in radiosensitivity. The results showed that M059J cells exhibited hyper-radiosensitivity compared with M059K cells. A strong G2 phase arrest was observed in M059J cells post irradiation. Significant accumulation in the G2 phase in M059J cells was accompanied by apoptosis at 12 h. Altogether, the data suggested that DNA-PK may have two roles in mammalian cells after DNA damage, a role in DNA DSB repair and a second role in DNA-damaged cells to traverse a G2 checkpoint, by which DNA-PK may affect cellular sensitivity to ionizing radiation. 地址: [Li Ning; Zhang Hong; Wang Yanling; Hao Jifang] Chinese Acad Sci, Inst Modern Phys, Lanzhou 730000, Peoples R China; [Li Ning; Zhang Hong; Wang Yanling; Hao Jifang] Key Lab Heavy Ion Radiat Med Gansu Prov, Lanzhou 730000, Peoples R China; [Li Ning; Wang Yanling] Chinese Acad Sci, Grad Sch, Beijing 100039, Peoples R China; [Wang Xiaohu] Gansu Tumor Hosp, Dept Radiotherapy, Lanzhou 730050, Peoples R China

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Little is known about the effects of space radiation on the human body. There are a number of potential chronic and acute effects, and one major target for noncarcinogenic effects is the human vasculature. Cellular stress, inflammatory response, and other radiation effects on endothelial cells may affect vascular function. This study was aimed at understanding the effects of space ionizing radiation on the formation and maintenance of capillary-like blood vessels. We used a 3D human vessel model created with human endothelial cells in a gel matrix to assess the effects of low-LET protons and high-LET iron ions. Iron ions were more damaging and caused significant reduction in the length of intact vessels in both developing and mature vessels at a dose of 80 cGy. Protons had no effect on mature vessels up to a dose of 3.2 Gy but did inhibit vessel formation at 80 cGy. Comparison with gamma radiation showed that photons had even less effect, although, as with protons, developing vessels were more sensitive. Apoptosis assays showed that inhibition of vessel development or deterioration of mature vessels was not due to cell death by apoptosis even in the case of iron ions. These are the first data to show the effects of radiation with varying linear energy transfer on a human vessel model. (C) 2011 In Radiation Research Society