Examination of the LBM in simulation of microchannel flow in transitional regime

The gas flows in micro-electro-mechanical systems possess relatively large Knudsen number and usually belong to the slip flow and transitional flow regimes. Recently the lattice Boltzmann method (LBM) was proposed by Nie et al. in Journal of Statistical Physics, vol. 107, pp. 279-289, in 2002 to simulate the microchannel and microcavity flows in the transitional flow regime. The present article intends to test the feasibility of doing so. The results of using the lattice Boltzmann method and the direct simulation Monte Carlo method show good agreement between them for small Kn (Kn = 0.0194), poor agreement for Kn = 0.194, and large deviation for Kn = 0.388 in simulating microchannel flows. This suggests that the present version of the lattice Boltzmann method is not feasible to simulate the transitional channel flow.

A scaling law of photoionization in few-cycle regime

In this paper, a scaling law of photoionization of atoms irradiated by intense, few- cycle laser pulses is established. The scaling law sets a relation to the phase- dependent ionization with the kinetic energy of photoelectrons, the duration and peak intensity of short pulses, and the ionization potential of the target atoms. We find that it will be advantageous to manifest the phase- dependent photoionization by choosing the target atoms with larger ionization potential, using laser with smaller carrier- frequency, and increasing the pulse intensity. (c) 2007 Optical Society of America.

Electron injection by a nanowire in the bubble regime

The triggering of wave-breaking in a three-dimensional laser plasma wake (bubble) is investigated. The Coulomb potential from a nanowire is used to disturb the wake field to initialize the wave-breaking. The electron acceleration becomes more stable and the laser power needed for self-trapping is lowered. Three-dimensional particle-in-cell simulations were performed. Electrons with a charge of about 100 pC can be accelerated stably to energy about 170 MeV with a laser energy of 460 mJ. The first step towards tailoring the electron beam properties such as the energy, energy spread, and charge is discussed. (C) 2007 American Institute of Physics.

Quantum path control in few-optical-cycle regime

We theoretically show that selection of a single quantum path in high-order harmonics generation can be realized in a few-optical-cycle regime with two-color schemes. We also demonstrate, in theory as well, the generation of spectrally smooth and ultrabroad extreme ultraviolet supercontinuum in argon gas which can produce single similar to 79 as pulses with currently available ultrafast laser sources. Our finding can be beneficial for generating isolated sub-100 as extreme ultraviolet pulses.

Bubble regime for ion acceleration in a laser-driven plasma

Proton trapping and acceleration by an electron bubble-channel structure in laser interaction with high-density plasma is investigated by using three-dimensional particle-in-cell simulations. It is shown that protons can be trapped, bunched, and efficiently accelerated for appropriate laser and plasma parameters, and the proton acceleration is enhanced if the plasma consists mainly of heavier ions such as tritium. The observed results are analyzed and discussed in terms of a one-dimensional analytical three-component-plasma wake model.

风和竞争对毛乌素沙地４种植物的影响

自然生境中，风是一种重要的生态/环境因子，已经引起生态学家的广泛兴趣。然而，目前对风和竞争如何共同影响植物行为的理解还很少。本文基于野外控制实验，研究赖草（Leymus secalinus）、黍（Panicum miliaceum）、油蒿（Artemisia ordosica）和雾冰藜（Bassia dasyphylla）四种沙生植物生长和形态特征对风和竞争的综合反应，以及降雨量变化是否修饰风和竞争的生态学效应。 风和竞争显著影响赖草和黍的生长和形态特征。赖草和黍的总生物量和分蘖数受密度效应影响较大，没有竞争的植株生物量和分蘖数都显著高于有竞争的植株。赖草和黍的根冠比和株高则受风因素的显著影响：风速越大，植株越趋向于降低株高并将更多的生物量分配到地下部分。除赖草株高显著外，竞争和风对两种植物生长和形态特征的交互作用不明显。 在风、竞争和水分实验中，风、竞争及其交互作用对油蒿和雾冰藜形态特征均有显著影响。油蒿株高在中风环境中最大，而雾冰藜株高在大风环境中最小;油蒿基径在弱风环境中最小，而雾冰藜则相反。种内竞争情况下的油蒿株高和基径显著高于种间竞争，而雾冰藜则相反。种内竞争情况下的油蒿株高和基径随风速的增大而减小;种间竞争情况下的油蒿株高和基径在弱风环境中最小，中等风区最大。油蒿和雾冰藜的分枝数都受竞争的显著影响，种间竞争情况下的油蒿分枝数显著高于种内竞争，而雾冰藜则相反。风显著影响油蒿的茎重比和雾冰藜的冠重比。油蒿的茎重比随风速的降低而降低。弱风环境中，雾冰藜的冠重比显著高于强风环境下的。风和竞争的交互作用显著影响油蒿生物量。种内竞争情况下，油蒿生物量在大风环境中最大，中风环境中最小;种间竞争情况下，油蒿生物量在中风环境中最大，弱风环境最小。水分显著影响油蒿的茎重比，以及雾冰藜的根冠比和基径，而对这两个种的其他生长和形态特征无显著影响。低水分情况下，油蒿的茎重比显著较高，雾冰藜的基径显著较低，并且分配更多生物量到地上部分。 这些结果初步表明，单优群落中的优势种或呈聚集分布的种群中，植株的生长符合“密度效应”原则，即密度越大，单株植物的生物量越小;并且在大风环境中，趋向于分配更多生物量到地下部分。种内竞争情况下油蒿幼苗的竞争能力强于种间竞争，这可能是自然群落中的油蒿不是聚集分布的一个原因。

毛乌素沙地四种关键植物幼苗出土及生长对沙埋和水分的响应

飞播是毛乌素沙地植被恢复与重建的重要手段。但此项技术仍存在一些问题，如飞播后成苗率较低等。柠条(Caragana korshinskii)、羊柴(Hedysarum laeve)、籽蒿(Artimisia sphaerocephala)与油蒿(Artimisia ordosica)是毛乌素沙地广泛分布的物种，也是飞播的主要物种。本文以飞播植被恢复技术为突破口，研究沙埋和土壤水分对种子萌发，幼苗出土和生长的影响，探讨幼苗出土和生长对沙生环境的适应对策。对采用合适的物种进行生态工程建设，提高生态工程的稳定性及可持续性具有重要意义。同时，本项研究有助于加深半干旱区植物对沙生环境适应机理的认识。 以上述4种植物为研究对象，设定7个沙埋深度和9个水分梯度，研究种子萌发和幼苗出土对沙埋和单次供水的响应。设定7个沙埋深度，选择3个沙丘部位，研究沙丘不同部位对植物种子萌发的影响。设定6个沙埋深度、4个水分梯度，研究两种蒿属植物幼苗生长对不同沙埋和供水的响应。得出如下主要结论： (1) 对于种子质量相对较大的柠条和羊柴而言，在一次性10-20 mm供水量条件下，幼苗主要在0.5-2 cm埋藏深度之间出土，但在埋藏深度为5 cm时这两个物种仍有少部分幼苗能够出土;对于种子质量相对较轻的油蒿和籽蒿而言，在一次性10-20 mm供水量时，幼苗主要在0.5 cm埋藏深度出土，油蒿和籽蒿幼苗在埋藏深度为1.5和2 cm时不能出苗。沙埋深度为0.5 cm时，4个物种出苗率较高、出苗时间较短、出苗速率较快。 (2) 实验期内(30天)在一次性供水量分别为5、7.5和7.5mm时，柠条、羊柴和油蒿出土幼苗全部死亡;在一次性供水量高于15-20 mm时，出土幼苗死亡率低于50%;籽蒿在供水量高于10 mm时出土幼苗死亡率低于50%;随供水量的增加4个物种出土幼苗的死亡率降低。 (3) 结合毛乌素沙地降雨特点与本文实验结果，0.5 cm的沙埋及7.5 mm以上的单次降雨量是上述4种植物自然条件下出苗较高的重要条件。 (4) 在沙丘顶部，2-7 cm沙埋深度之内各个物种不同沙埋深度的种子萌发率差异不显著。沙丘背风坡中部和底部，4个物种在沙埋深度为1 cm时的种子萌发率均显著高于5、7 cm时的萌发率。当沙埋深度为1-5 cm时，柠条和羊柴种子在坡面不同位置的萌发率均高于20%，且显著高于7 cm沙埋深度时的萌发率。在背风坡底部时，柠条、羊柴、油蒿和籽蒿的种子萌发率达到最大值，分别为45.2±3.27%、48.4±5.21%、20.8±4.63%和22.4±4.83%。4个物种的种子萌发率从沙丘顶部到背风坡中部到底部呈递增趋势，表明背风坡中部和底部的环境条件要比顶部更适合种子萌 发。 (5) 部分沙埋促进幼苗生长。2种蒿属植物幼苗在沙埋深度为0.25、0.5 H时比在0、0.75 H时具有更高的生物量、叶面积、相对生长速率（RGR）和净同化速率（NAR）。在75 mm/月供水量时，油蒿幼苗具有较高的生物量和叶面积，但当供水量达到100 mm/月时其幼苗生长受到抑制。油蒿幼苗在遭遇较深（0.5、0.75 H）沙埋时的根冠比要显著高于未沙埋幼苗的根冠比;籽蒿幼苗根冠比在不同沙埋条件下没有显著变化。籽蒿幼苗在50 mm供水量时具有较高的RGR。油蒿幼苗在75 mm供水量时具有较高的RGR和NAR。

EXPERIMENTS ON AQUATIC ECOSYSTEM REGIME SHIFT IN ENCLOSURES NEAR LAKE DIANCHI, CHINA

To discover how a lake converts from a turbid state to clean state, and what drives this process, we constructed controlled enclosure ecosystems and used the ecological remediation method to force ecosystems to convert from the turbid state to the clean state. Our results show that the driving forces include temperature., macrophyte, silver carp and mussel, which form a combined force to drive the controlled ecosystem to switch. There is a threshold existing in treated enclosure ecosystem during the conversion from turbid to clean state. When TP <0.09 mg.L-1, Chl-a <0.036 mg.L-1, transparency >62 cm, TN <2.15 mg.L-1, CODMn <13.7 mg.L-1, tubidity <10, and the number of algal cells <10(6) cells.L-1, the treated ecosystem changes sharply from turbid to clean state. The conversion process can be divided into three phases: turbid state, clean-turbid transitional state as well as clean state, and described with the power function Y = a*X-b (where Y is water parameter, X is time, a and b are constants), which indicates that the shift in the enclosure ecosystem from turbid to clean state is discontinuous.