956 resultados para Ellberbe, L. W.


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无根萍属(Wolffia )隶属于浮萍科天南星目,是世界上最小的被子植物。该属植物繁殖速度快;易于培养;结构简单,只具有一个雄蕊和一个雌蕊;自然状态下通常为克隆繁殖,遗传结构高度一致,具备特定研究目的模式植物的特点,正在或已经成为一些实验室研究光合作用、生物反应器、毒理学、生态修复和环境监测等的重要模式生物材料;同时还被作为建造航天生活仓和地外生命支撑系统的首选植物。该属植物蛋白含量高且氨基酸组分平衡,营养价值可与大豆相媲美。但该属植物一直是分类学界的疑难类群,不同的学者对该属的分类处理比较混乱;其次,对该属的生物地理研究也很不够,尤其是对国产类群的研究;另外,W. globosa 作为该属中国分布的物种,其生理学特性和形态结构发育还缺乏研究。为此,本文通过mat K 基因测序、RAPD 标记等手段,结合野外和室内的长期观测,对其分类和中国的地理分布以及生理学特性进行了研究。针对浮萍科植物作为水生植物,其对重金属和芳香烃衍生物的耐受逆境能力大小,和对淡水水体环境生态的指示作用。本文研究了W. globosa 具解毒功能的谷胱甘肽转硫酶的活性;最后,探索了从黄鳝(Monpterus albus Zuiew )中分离纯化GSTs 的技术与方法并对maGST 的部分特性进行了研究。主要研究结果如下: 1. Wolffia 系统分类学研究 前人认为,Wolffia 柱头的颜色是重要的分组、分种检索性状。我们对其长期、活体、原位、实时跟踪观测结果表明,柱头颜色是Wolffia 个体发育上的变化过程,不是一个稳定性状,用作Wolffia subgroup 内组的划分特征和种的鉴别特征是不适合的。在此基础上我们重新修定了该属的分种检索表。利用形态分类学性状——气孔、长/宽、高/宽以及最大宽度在水面上还是水面下等性状,认为中国分布的类群应是W. globosa,但亦有W. neglecta 存在的证据。mat K 基因片段结果支持形态学的结论。通过广泛的野外采集,在我国北京、河北和吉林发现Wolffia 的新分布。 2. 中国Wolffia 居群遗传学研究 以RAPD 分子标记对广泛分布的居群遗传多样性研究表明,无根萍属植物主要以无性繁殖方式繁育,居群主要由单一克隆后代组成,如海河流域以及松花江流域居群;但一些居群亦兼有性繁殖方式,并具较高的遗传多样性,如武汉、海南居群。利用MVSP, Popgene 和Ntsys 等分析方法探讨了中国产Wolffia 居群遗传多样性和地理分布格局间关系。 3. W. globosa 的生理学研究 建立了较为完善的W. globosa 的无菌培养和保存体系。W. globosa 在逆境中,会形成休眠体;同时,发现不同居群甚至不同克隆系之间其抗逆性和生长速度存在着显著差异,差异最大的如海南文昌居群的生长速率,是长春居群的4.19 倍;不同的时间统计生长周期存在着不同结果,生长节律每天有两个生长高峰呈双“S”型;W. globosa 的耐受温度范围和pH 范围广;低浓度的IAA,GA,6-BA, EDDHA-Fe 以及EDTA 等物质具有促进W. globosa 生长的特性;但是,所有这些处理均没能促使W. globosa 从营养生长转入生殖生长。 4. W. globosa 的解剖学研究 W. globosa 通常是进行克隆繁殖,通过组织切片发现无性分枝子体还未伸出母株之前就已经完成分化,与此同时分枝子体中又分化出新的子体,分枝呈聚伞状,子体生长方向彼此相对;另外,生殖生长结构的分化也是在母体中完成的;生殖生长点与营养生长点不是同一生长点。 5. 浮萍科植物的毒理学研究 以重金属Cr3+和芳香烃衍生物CDNB 溶液处理Wolffia,SpirodelaLemna, 三种水生生物,结果表明Wolffia 比SpirodelaLemna 对重金属和芳香烃衍生物有更强的抗逆能力,如在同等条件下对于Cr3+Wolffia 的半致死剂量800GB(≈ 80mg/L),而SpirodelaLemna 则分别为10mg/L;20mg/L;表明W. globosa 是一个优良的生态环境修复植物。与此同时,研究了W. globosa 中具有解毒功能的GSTs 粗酶液活力在不同浓度的重金属离子(Cu2+和Cd2+)以及芳香烃衍生物(CDNB 和NBD-Cl随处理时间的变化情况。 6. 从水生生物黄鳝Monpterus albus Zuiew 中分离纯化GSTs 的研究GSTs 活性的变化是环境监测的一个Biomarker,为此研究从M. albus 中分离 纯化GSTs 的技术与方法。经GSH 亲和层析纯化的酶活力为粗酶液的207 倍,进而鉴定了maGST 的部分特性。SDS-PAGE 电泳和MALDI-TOF/MS 表明MaGST 为同源二聚体,分子量约为52kDa,单亚基分子量约为26 kDa。maGST 酶动力学表明对CDNB 为13.07 ± 0.37 微摩尔每分钟每毫克蛋白;对NBD-Cl 为5.54 ± 微摩尔每分钟每毫克蛋白;对ECA、4-NPA 几乎没有活性。在GSH 底物饱和,CDNB 的Km 值和Vmax 分别为0.32 mM 和16.19 微摩尔每分钟每毫克蛋白;CDNB 底物饱和,GSH 的Km 值和Vmax 分别为0.44 mM 和28.83 微摩尔每分钟每毫克蛋白。maGST 的酶活性pH 值较宽,温度范围广:在pH7.0-7.5 具有最大速度,在pH6.5 和pH8.5 时分别具有65%和72%的酶活力;在45℃时具有最大活性,30℃和55℃时为最大活力的80%,60℃几乎完全丧失酶活力。

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槽舌兰属为(Holcoglossum schltr.)兰科树兰亚科万代兰族指甲兰亚族植物,大部分种类为中国特有种,部分种类分布到越南、泰国、缅甸等国家和地区。本研究利用ITS、trnL-F和matK序列重建了槽舌兰属的系统树,在此基础上对其和植物地理进行了初步探讨并对该属植物的叶表皮特征演化进行了探讨。具体结果如下: 1.槽舌兰的分子系统学研究及分子植物地理学 对槽舌兰属的13个种的12个种进行了取样(H. quasipinifolium未包括),而横断山地区所有已知的槽舌兰属植物的居群进行了取样,共有25个取样代表了槽舌兰属。运用ITS、trnL-F和matK序列重建了槽舌兰属的系统树。槽舌兰属得到了很强的单系支持,并且分为了从南到北的三个分支,其中高山类群得到了很强的支持,尽管该类群内部系统关系没有得到解决。本研究推测槽舌兰属是从南部的热带地区向北部扩散,并在横断山地区辐射分化。槽舌兰高山类群的辐射分化和该地区的迅速隆起密切相关。 2.槽舌兰属的叶表皮演化 在光学显微镜下和电子显微镜下,观察了21个代表槽舌兰属8个种以及5个来自Vanda concolor和 Aerides ordorata的叶表皮样品的常规特征,包括表皮细胞的形状,密度,垂周壁式样,气孔类型,气孔指数,气孔长/宽(L/W, 气孔大小等等。槽舌兰属的气孔除H. omeiense外,其它上、下表皮均有气孔分布,是比较进化的类型。表皮细胞为多边形,垂周壁平直或弓形。槽舌兰属的上表皮细胞都大于下表皮的细胞。与万代兰族的其它类群相似。结果表明,气孔类型和气孔指数与属的系统发育关系一致,可以作为一个很好的特征。 3.槽舌兰属高山组的物种形成初探 槽舌兰属高山组植物在形态上、传粉系统以及生境都有了很大的分化,但该类群在分子序列上却几乎没有区别,本文推测该类群是近期的辐射分化形成的。

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The paper deals with the spawning cycle of the hake, Merluccius merluccius hubbsi in the fishing area of the Argentine fleet, SW Atlantic (35°- 46° L. S.: 53°- 63° L.W.; 30-160 fathoms depth). It was made on the basis of the weekly sampling of the commercial catch in the period January 1965 - March 1968. The results have been compared with those of the exploratory surveys made by the United Nations Fisheries Development Program (República Argentina - FAO). The histological study, which was made with 741 specimens, was most intensive in females than in males. The results have been compared with the sexual stage determinations of both sexes in the total samples during the period before mentioned. The conclusions are: 1. The analysis of the ovocytes frequency distributions showed a period of resting or slow recuperation (April - August) with a mode of 120 ~k and one of rapid transformation (October - December) from 120 μ tíll 830 ~k. After December it appears again the mode of 120 ~k which indicated the reserve stock. 2. The maturity factor shows in both sexes a period of low values , 0,52 to 2% (April - September) and, another with higher values (October - March). In the first period the values are concentrated, while in the second one a large dispersion is observed produced by the rapidity of the growth process of the gonads. It is more evident between November and December. 3. The liver weight variations, compared with the degree of ingestion and the values of the maturity factor, in time, demonstrated that: a) after two periods of abundant ingestion (March - April and October- November) there are two increases of the liver index; b) the increase of the Iiver index has a direct relation to the maturity factor; c) at the end of the summer season, when the values of the maturity factor decrease, those of the liver index are still high. This demonstrates that the hake does not arrive exhausted at the end of the spawning season and that a rapid recuperation for a new spawning by part of the stock is possible. 4. Females predominate in the samples during most of the year. In the period October - December, when sexual activation occurs, as it is demonstrated by the high values of the maturity factor, proportions are nearly 1 :1, and males at times are more numerous than females. 5. The analisys of the advaneed maturity stages, in relation to total length shows that in the hake, Iike in other fishes, the largest ones mature first. This applies for both sexes. 6. The study of the maturity factor values and the sexual stages of the samples allows the recognition of two spawning periods, the main one in summer (October - March) and another in winter (June - July). 7. Part of the summer spawners, with a rapid recuperation, should be able to spawn again in winter. This indicates that the hake population, acording to our samples, has two different possibilities of spawning. 8. After analysis of the frequency percentages composition of mature specimens it is concluded that during the summer season, when hake is fished in shallow waters and in a wide area (38°– 43° L.S.) the fleet is fishing on the spawning stocks. Some winter spawners specimens have been found at 37°- 38° L.S. and in waters of more than 100 fathoms depth. 9. A new maturity scale of seven stages is proposed, instead of the one of six stages now in use. The new added stage corresponds to the postspawners during its resting period.

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The turbulent drag reduction due to riblets is a function of their size and, for different configurations, collapses well with a length scale l+g=(A+g)1/2, based in the groove cross-section Ag. The initially linear drag reduction breaks down for l+g≈11, which agrees in our DNS with the previously reported appearance of quasi-two-dimensional spanwise rollers immediately above the riblets. They are similar to those found over porous surfaces and plant canopies, and can be traced to a Kelvin-Helmholtz-like instability associated with the relaxation of the impermeability condition for the wall-normal velocity. The extra Reynolds stress associated with them accounts quantitatively for the drag degradation. An inviscid model for the instability confirms its nature, agreeing well with the observed perturbation wavelengths and shapes. The onset of the instability is determined by a length scale L+w that, for conventional riblet geometries, is proportional to l+g. The instability onset, L+w4, corresponds to the empirical breakdown point l+g≈11.

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We demonstrate that a p-n junction created electrically in HgTe quantum wells with inverted band structure exhibits interesting intraband and interband tunneling processes. We find a perfect intraband transmission for electrons injected perpendicularly to the interface of the p-n junction. The opacity and transparency of electrons through the p-n junction can be tuned by changing the incidence angle, the Fermi energy and the strength of the Rashba spin-orbit interaction (RSOI). The occurrence of a conductance plateau due to the formation of topological edge states in a quasi-one-dimensional (Q1D) p-n junction can be switched on and off by tuning the gate voltage. The spin orientation can be substantially rotated when the samples exhibit a moderately strong RSOI.

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Based on the effective-mass model, the lower energies of the electron and the hole of ZnO/MgxZn1-xO superlattices are calculated. Because of the mismatch of the lattice constant between the ZnO well and the MgxZn1-xO barrier, piezoelectric and spontaneous polarization exist in ZnO/MgxZn1-xO superlattices and a macroscopical internal electric held is found when well width L-w >4 nm and Mg concentration x > 0.2. The parameters of ZnO/MgxZn1-xO superlattices such as lattice constant, band offset, etc. are also proposed. Through calculations, we found the internal electric field can change the lowest energies of the electron and hole to 105.4 and 85.1 meV when well width L-w up to 70 angstrom, which will influence the electronic and optical properties of ZnO/MgxZn1-xO superlattices greatly, while the Rashba effect from the internal electric field is so small that it can be neglected. The ground state exciton energies with different Mg concentration x are also calculated by variational method, our results are very close to the experimental results when Mg concentration x <= 0.3. (C) 2008 Elsevier B.V. All rights reserved.

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Double-state lasing phenomena are easily observed in self-assembled quantum dot (QD) lasers. The effect of inter-level relaxation rate and cavity length on the double-state lasing performance of QD lasers is investigated on the basis of a rate equation model. Calculated results show that, for a certain cavity length, the ground state (GS) lasing threshold current increases almost linearly with the inter-level relaxation lifetime. However, as the relaxation rate becomes slower, the ratio of excited state (ES) lasing threshold current over the GS one decreases, showing an evident exponential behavior. A relatively feasible method to estimate the inter-level relaxation lifetime, which is difficult to measure directly, is provided. In addition, fast inter-level relaxation is favorable for the GS single-mode lasing, and leads to lower wetting layer (WL) carrier occupation probability and higher QD GS capture efficiency and external differential quantum efficiency. Besides, the double-state lasing effect strongly depends on the cavity length. (c) 2007 Elsevier B.V. All rights reserved.

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In this review, the potential of mode-locked lasers based on advanced quantum-dot ( QD) active media to generate short optical pulses is analysed. A comprehensive review of experimental and theoretical work on related aspects is provided, including monolithic-cavity mode-locked QD lasers and external-cavity mode-locked QD lasers, as well as mode-locked solid-state and fibre lasers based on QD semiconductor saturable absorber mirrors. Performance comparisons are made for state-of-the-art experiments. Various methods for improving important characteristics of mode-locked pulses such as pulse duration, repetition rate, pulse power, and timing jitter through optimization of device design parameters or mode-locking methods are addressed. In addition, gain switching and self-pulsation of QD lasers are also briefly reviewed, concluding with the summary and prospects.

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The magnetoexciton polaron (MP) is investigated theoretically in a diluted magnetic semiconductor quantum dot (QD), with the Coulomb interaction and the sp-d exchange interaction included. The MP energy decreases rapidly with increasing magnetic field at low magnetic field and saturates at high magnetic field for small QDs, and the dependences of the MP energy on magnetic field are quite different for different QD radii due to the different carrier-induced magnetic fields B-MP. The competition between the sp-d exchange interaction and the band gap shrinkage results in there being a maximum exhibited by the MP energy With increasing temperature. Our numerical results are in good agreement with experiment (Maksimov A A, Bacher G, MacDonald A, Kulakovskii V D, Forchel A, Becker C R, Landwehr G and Molenkamp L W 2000 Phys. Rev. B 62 R7767).