Use of PFU protozoan community structural and functional characteristics in assessment of water quality in a large, highly polluted freshwater lake in China

Structural and functional parameters of protozoan communities colonizing on PFU (polyurethane foam unit) artificial substrate were assessed as indicators of water quality in the Chaohu Lake, a large, shallow and highly polluted freshwater lake in China. Protozoan communities were sampled 1, 3, 6, 9 and 14 days after exposure of PFU artificial substrate in the lake during October 2003. Four study stations with the different water quality gradient changes along the lake were distinguishable in terms of differences in the community's structural (species richness, individual abundance, etc.) and functional parameters (protozoan colonization rates on PFU). The concentrations of TP, TN, COD and BOD as the main chemical indicators of pollution at the four sampling sites were also obtained each year during 2002-2003 for comparison with biological parameters. The results showed that the species richness and PFU colonization rate decreased as pollution intensity increased and that the Margalef diversity index values calculated at four sampling sites also related to water quality. The three functional parameters based on the PFU colonization process, that is, S-eq, G and T-90%, were strongly related to the pollution status of the water. The number of protozoan species colonizing on PFU after exposure of 1 to 3 days was found to give a clear comparative indication of the water quality at the four sampling stations. The research provides further evidence that the protozoan community may be utilized effectively in the assessment of water quality and that the PFU method furnishes rapid, cost-effective and reliable information that may be useful for measuring responses to pollution stress in aquatic ecosystems.

Strength and hydration products of reactive MgO-silica pastes

The reaction between MgO and microsilica has been studied by many researchers, who confirmed the formation of magnesium silicate hydrate. The blend was reported to have the potential as a novel material for construction and environment purposes. However, the characteristics of MgO vary significantly, e.g., reactivity and purity, which would have an effect on the hydration process of MgO-silica blend. This paper investigated the strength and hydration products of reactive MgO and silica blend at room temperature up to 90 days. The existence of magnesium silicate hydrate after 7 days' curing was confirmed with the help of infrared spectroscopy, thermogravimetric analysis and X-ray diffraction. The microstructural and elemental analysis of the resulting magnesium silicate hydrate was conducted using scanning electron microscopy and energy dispersive spectroscopy. In addition, the effect of characteristics of MgO on the hydration process was discussed. It was found that the synthesis of magnesium silicate hydrate was highly dependent on the reactivity of the precursors. MgO and silica with higher reactivity resulted in higher formation rate of magnesium silicate hydrate. In addition, the impurity in the MgO affects the pH value of the blends, which in turn determines the solubility of silica and the formation of magnesium silicate hydrate. © 2014 Elsevier Ltd. All rights reserved.

Growing 20 cm Long DWNTs/TWNTs at a Rapid Growth Rate of 80-90 mu m/s

Submitted by 阎军 (yanj@red.semi.ac.cn) on 2010-04-13T16:03:37Z No. of bitstreams: 1 Growing 20 cm Long DWNTsTWNTs at a Rapid Growth Rate of 80-90 mu ms .pdf: 3229914 bytes, checksum: 0259795afb443dc6901c11df5ecd325a (MD5)

Optical properties of alloy states in GaNxAs1-x (x < 0.01)

A set of GaNxAs1-x samples with a small content of nitrogen (N) (< 1%) were investigated by continuous-wave photoluminescence (PL), pulse-wave excitation PL, and photo reflectance technology. Temperature-and excitation-dependence of PL disclosed the intrinsic band gap properties of alloy states in GaNxAs1-x, which was extremely different from the N-related impurity states. At the same time, PR spectra were also studied in this work.

Calculation of energy levels in InGaAs/GaAs quantum dot array

The subbands of the ground state E-c1, the first excited state E-c2 and heavy hole state E-HH1 are calculated by solving the eigenvalues of effective-mass Hamiltonian H-0 which is derived from eight-band k . p theory and the calculations are performed at k(x) = k, = k = 0 for the three-dimensional array of InGaAs/GaAs quantum dots (QDs). With indium content in InGaAs QDs gradually increasing from 30% to 100%,the intersubband transition wavelength of E-c2 to E-c1, blue-shifts from 18.50 to 11.87 mu m,while the transition wavelength of E-c1, to E-HH1, red-shifts from 1. 04 to 1. 73 mu m. With the sizes of Ir-0.5 Ga-0.5 As and InAs QDs increasing from 1.0 to 5.0 nm, the intersubband transition from E-c1, to E-C2 transforms from bound-state-to-continuum-state to bound-state-to-bound-state, and the corresponding intersubband transition wavelengths red-shift from 8.12 pm (5.90 pm) to 53.47 mu m (31.87 pm), respectively, and the transition wavelengths of E-C1 to E-HH1 red-shift from 1. 13 mu m (1.60 mu m) to 1.27 mu m (2.01 mu m), respectively.

Silicon thin films prepared in the transition region and their use in solar cells

Diphasic silicon films (nc-Si/a-Si:H) have been prepared by a new regime of plasma enhanced chemical vapour deposition in the region adjacent of phase transition from amorphous to microcrystalline state. Comparing to the conventional amorphous silicon (a-Si:H), the nc-Si/a-Si:H has higher photoconductivity (sigma(ph)), better stability, and a broader light spectral response range in the longer wavelength range. It can be found from Raman spectra that there is a notable improvement in the medium range order. The blue shift for the stretching mode and red shift for the wagging mode in the IR spectra also show the variation of the microstructure. By using this kind of film as intrinsic layer, a p-i-n junction solar cell was prepared with the initial efficiency of 8.51 % and a stabilized efficiency of 8.01% (AM 1.5, 100 mw/cm(2)) at room temperature. (c) 2006 Published by Elsevier B.V.

Silicon thin films prepared in the transition region and their use in solar cells

Diphasic silicon films (nc-Si/a-Si:H) have been prepared by a new regime of plasma enhanced chemical vapour deposition in the region adjacent of phase transition from amorphous to microcrystalline state. Comparing to the conventional amorphous silicon (a-Si:H), the nc-Si/a-Si:H has higher photoconductivity (sigma(ph)), better stability, and a broader light spectral response range in the longer wavelength range. It can be found from Raman spectra that there is a notable improvement in the medium range order. The blue shift for the stretching mode and red shift for the wagging mode in the IR spectra also show the variation of the microstructure. By using this kind of film as intrinsic layer, a p-i-n junction solar cell was prepared with the initial efficiency of 8.51 % and a stabilized efficiency of 8.01% (AM 1.5, 100 mw/cm(2)) at room temperature. (c) 2006 Published by Elsevier B.V.

La2Zr2O7的增韧及陶瓷纤维的制备

La2Zr2O7是一种近年来才提出的新型热障涂层材料，该材料熔点高，在熔点以下不发生相变，热导率低，抗烧结及没有氧传输发生，这些特点使得它作为一种高温下应用的热障涂层材料越来越引起人们的重视。但是，由于该材料的热膨胀系数和断裂韧性比较低，它的实际应用受到了限制。 在本论文中，使用高压烧结的方法获得了致密化的纳米La2Zr2O7块体材料，并对其断裂韧性和热膨胀系数进行了研究。得到的La2Zr2O7纳米材料的断裂韧性和热膨胀系数分别为1.98MPam1/2和9.6×10-6K-1 (200-1000℃)，这些数值明显高于非纳米的La2Zr2O7陶瓷(断裂韧性和热膨胀系数分别为1.40 MPam1/2 和 9.1×10-6 K-1，该结果表明纳米化是一种提高材料断裂韧性和热膨胀系数的有效方法。在La2Zr2O7纳米粉末中加入8YSZ纳米颗粒，高压烧结后使其颗粒充分生长，在得到的复相化合物中观察到形成了类似棒状晶体的自增韧相，使得复合材料的断裂韧性(1.88 MPam1/2)比La2Zr2O7有所提高，甚至超过了同样条件下制备的8YSZ样品的断裂韧性。 La2Zr2O7的断裂韧性也可以通过在基体中添加BaTiO3铁电材料得到明显的提高。当添加BaTiO3的体积含量达到10vol％时，4.5GPa，1450℃高压烧结10min得到的复合材料断裂韧性达1.98 MPam1/2，明显高于同条件下烧结的La2Zr2O7 (1.60MPam1/2)。应力诱导下BaTiO3的电畴转向是主要的增韧原因。随着BaTiO3颗粒添加的体积含量增加，复相化合物的热膨胀系数也明显提高。当掺杂20vol％BaTiO3时，得到的复合材料平均热膨胀系数达到10.2×10-6K-1 (150~1200℃)。 我们通过在4.5GPa, 1650℃高压烧结5min的方法还获得了掺杂YAG纳米颗粒的La2Zr2O7纳米复相陶瓷。在室温下测量了材料的维氏硬度，并通过压痕裂纹长度计算出了材料的断裂韧性。随着YAG纳米颗粒体积含量的增加，纳米复相陶瓷的断裂韧性和维氏硬度都依次增加，当添加20vol％的YAG纳米颗粒时达到最大，分别为1.93 MPam1/2和11.45GPa。断裂韧性增加的机理可归结为以下三点：一是YAG纳米颗粒的添加提高了La2Zr2O7基体的晶界强度，二是基体晶粒尺寸变化的影响，三是YAG纳米颗粒对裂纹的偏转和钉扎作用。添加微米YAG颗粒的复相化合物因为和纳米复相陶瓷具有不同的增韧机制，因此断裂韧性的变化趋势也不相同，在掺入10vol％的YAG微米颗粒时，复合材料的断裂韧性最大，而后降低，当掺入YAG微米粒子的体积含量达到20vol％时，断裂韧性甚至低于La2Zr2O7。 从20世纪90年代开始，电纺作为一种合成纤维的办法越来越吸引人们的注意。其合成的纤维长度长，直径均匀，并且组成范围很广。最初，电纺只是被用来合成一些有机聚合物的纤维，最近，很多研究组开始致力于使用电纺的方法合成复合纤维或者陶瓷纤维。 在本论文中，我们使用电纺的方法获得了La2Zr2O7纳米纤维和SiC单晶纳米线。1000℃煅烧得到的La2Zr2O7纳米纤维具有烧绿石结构，直径在200~500nm之间。同样的温度煅烧时得到的La2Zr2O7纳米纤维的比表面积要明显高于粉末样品的，表明纤维的抗烧结性能比粉末的高。得到的SiC纳米线直径在50~100nm之间，表面有一约5nm厚的无定形的SiO2薄层。 使用电纺的方法，恰当的控制煅烧条件，我们获得了La2Ce2O7， La2(Zr0.745Ce0.386)2O7.524和8YSZ中空纤维。这种中空结构减小了粒子之间的接触面积，提高了材料的抗烧结性能。在扫描电镜分析的基础上，我们总结了这些中空纤维的形成过程。

塔城黑白仰鼻猴（Rhinopithecus bieti）的觅食生态学和社会

从 1999 年4 月至2002 年六月间，对黑白仰鼻猴种群(Rhinopithecus bieti ) 的分布和生境状况进行了调查。与十年前的调查结果相比，本次调查新发现了4 个亚种群（指存在生境走廊的若干群体），但有5 个以前存在的群已经消失，现 存猴群数量为13 群，总体数量约为1200-1700 只。从西藏的芒康到云龙的龙马 山，随着海拔的降低，猴群可利用的植被类型也随之多样化。但由于砍伐、放牧、 开矿等因素的影响，猴群生境破碎化程度较高，连接猴群的生境走廊状况极差， 多数猴群孤立分布，并且存在小种群问题，生境走廊的维护和恢复已成为该物种 保护成功与否的关键。种群的总体数量下降了32%（不含4 个新发现的亚种群）， 其中4 群数量下降，4 群持平，1 群有所增长，5 群消失，这不容乐观的状况给 我们保护敲响了警钟。此外，基于以前的研究结果，暗针叶林、针阔混交林和栎 树林均为其适宜生境，夏季高山牧场则是由当地居民为放牧而砍伐、焚烧高海拔 带的暗针叶林而形成的林间空地。我们使用了1997 年的卫星影像和1958 年的航 拍地图来估算适宜生境和夏季高山牧场的面积。结果表明；1）在1997 年，黑白 仰鼻猴的适宜生境面积为4169 km2，夏季高山牧场的面积为1923 km2。2）在近 40 年中，黑白仰鼻猴的适宜生境面积下降了31％（约1887 km2），而夏季高山牧 场的面积则增加了204％（约1291 km2）。3）森林斑块的平均面积从15.6 km2 下降到5.4 km2。此外，夏季高山牧场的面积与当地居民的人口数量增长之间呈 正相关关系 (R2 ≥ 0.53，p < 0.05)。除非当地居民的人口数量增长模式或者传统 的生产生活方式发生改变，这种破碎化趋势将继续下去。 从1999 年三月至2000 年十二月对云南塔城(99o18’E, 27 o36’N, 活动范围在 2,700 – 3700 m asl)的一群黑白仰鼻猴收集了食性和时间预算的数据。通过状态 行为扫描的方式，主要记录了树冠中单雄组食用植物种类—部位。同时用显微镜对每个月的粪便样本进行了显微分析，以此作为食性的补充数据。仰鼻猴食用属 于28 科、42 属的59 种植物，共计90 个食用的植物种类—部位，其中冬季利用 21 个植物种类—部位，春季38 个，夏季39 个，秋季47 个。另一方面，该群年 平均花费日活动时间的35％进食，33％休息，15％移动，13％社会行为。日活 动时间预算分配、摄食不同食物类别的时间、粪便中食物残留物及食用植物种 类―部位的数目存在着季节性变化。食物种类与时间分配之间和之内的相关显然 是为了最大化觅食效率与最小化能量消耗。考虑到来自北面与南面的群的相关报 道，这个种对生境的适应性似乎与其他疣猴没什么区别，并无特化之处。因此， 这个种的最终生存预期要比以前乐观。 我们利用整个塔城猴群沿地面通过开阔地或喝水的机会，使我们能记录野外 种群的大小和组成（如性比等）以及通过分析依次经过个体间的时间间隔以量化 反映社会组织单元之间和之内的空间距离，用统计分析的方式来量化描述社会组 织的模式，发现塔城猴群由9 个单雄单元（OMUs）、5 个多雄单元（MMUs）和2 个全雄单元（AMUs）组成， 单雄单元、多雄单元和全雄单元内的个体分别约占 总数的58％、34％和8％，无论在开阔峡谷地域或水潭旁，单元内的时间间隔显 著短于单元间的时间间隔（开阔峡谷地域：非配对 t 检验，df = 49; p < 0.01， 水潭：非配对t 检验，df = 35; p < 0.01）。 在单雄单元的成年不等性比和成 年雌性与婴猴的比例显著大于多雄单元（开阔峡谷地域：非配对t 检验，df = 40; p < 0.05，水潭：非配对t 检验，df = 16; p < 0.05）。在全雄单元中有大量的 性别不明的未成年个体。此外，加之某些个案描述，论述了多雄单元存在的可能 性及与全雄单元和单雄单元之间的关系。

INFLUENCE OF THE 90-DEGREES PARTIAL DISLOCATION CORE STRUCTURE IN SILICON ON ENERGY-LEVELS

An LCAO-scheme taking into account 10 atomic orbitals (s-, p-, and d-type) is used to calculate the electronic structure of the reconstructed 90-degrees partial dislocation in Si. Two different valence force fields producing deviating results are used for modelling the core structure. Geometrical data published by another group is also used. The aim is to explore the influence of geometry on energy levels. We find that the band structure depends sensitively on bond angles. Using data determined by the Tersoff potential we obtain two bands of which the upper one penetrates deeply into the indirect band gap while the geometry minimizing the simple Keating potential leaves the gap completely clear of dislocation states. Thus, from a theoretical point of view, the chief difficulty in calculating the electronic structure of the reconstructed 90-degrees partial is the lack of accurate structural information.

ENERGY-LEVEL CALCULATIONS OF THE RECONSTRUCTED 90-DEGREES PARTIAL DISLOCATION IN SILICON

An LCAO scheme taking into account 10 atomic orbitals (s-, p-, and d-type) applied to a supercell containing 256 atoms is used to calculate the bound states of the reconstructed 90-degrees partial dislocation in Si. The results differ significantly from our earlier calculations on the unreconstructed 90-degrees partial using the same method. We find two bands separate from each other in the entire Brillouin zone and the upper band penetrates deep into the indirect band gap which is in contradiction with the general opinion that core reconstruction clears the band gap of dislocation states.

ELECTRON-STATES OF A VACANCY IN THE CORE OF THE 90-DEGREES PARTIAL DISLOCATION IN SILICON

An LCAO scheme (linear combination of atomic orbitals) taking into account ten atomic orbitals (s-, p-, and d-type) is used to calculate the electronic structure of a vacancy present in the core of the reconstructed 90 degrees partial dislocation in silicon. The levels in the band gap are extracted using Lanczos' algorithm and a continued fraction representation of the local density of states. The three-fold degenerate stale of the ideal vacancy is split into three levels with energies 0.26, 1.1, and 1.9 eV measured from the valence band edge.