地下爆炸Rg波低谷点激发机理

目前普遍认为Rg_S散射是地下核爆炸短周期Lg波的主要能量来源,其主要依据为由线性偶极补偿源（CLVD）激发的Rg波谱的低谷点随深度变化的特征与区域震相Lg波谱的低谷点随深度变化的特征具有一致性. 本文利用简正振型理论,分析了Rg波谱中低谷点的形成机理,给出了各种速度模型下CLVD源深度与低谷点频率之间的关系,并分析了利用公式hCLVD=V/(16fNull)估计震源深度的局限性. 本文的研究结果进一步支持了CLVD源是激发Lg波的主要因素的观点,并得到重要结论：CLVD源形式下的本征位移函数及其导数的叠加所形成的极小值,即源的空间分布特征,是形成Rg波低谷点的原因,而不能仅用水平向基频本征位移函数过零点来解释.     

地下核爆炸Lg波的激发机制

地下核爆炸Lg波的激发机制,目前尚未十分清楚.其中主要观点之一是源区附近由补偿线性矢量偶极源（CLVD）激发的Rg波的散射形成的S波是Lg波能量的主要来源.本文利用理论地震图模拟方法,基于东哈萨克斯坦地区速度模型,分析比较了东哈萨克斯坦地壳速度模型下的爆炸源、张裂源及CLVD源对区域震相Lg波的影响.结果表明,从能量的角度来看,CLVD源是激发Lg波的主要因素.模拟计算结果也进一步证实了CLVD源激发的Lg波振幅谱具有低谷点的特征源自于该震源所激发的Rg波;在此基础之上,检验了Patton提出的估算震源埋藏深度的经验公式.结果发现,该公式仅适用于震源埋藏深度较浅的情况（<500m）.这些结果对于进一步理解及更好地利用Lg波具有重要理论指导意义.     

Ring-Shaped Jets in Gamma-Ray Bursts

When the axis of a gamma-ray burst (GRB) does not coincide with the spin axis of its source, there may result a ring-shaped jet. Using some refined jet dynamics, we calculate multi-wavelength afterglow light curves for such ring-shaped jets. In the R-band we find an obvious break in the afterglow light curve due to the beaming effect and the break is affected by many parameters, such as the electron energy fraction ξe, the magnetic energy fraction ξ2B, the width of ring A0 and the medium number density n. The overall light curve can be divided into three power-law stages, I.e., an ultra-relativistic stage, an after-break stage and a deep Newtonian stage. For each stage the power-law index is larger in the ring-shaped jet than in the corresponding conical jet.     

南极中山站至Dome A考察断面湍流参数特征近地层湍流参数特征

利用南极中山站至Dome A考察断面上3个自动气象站2005～2007年的观测资料和2008年夏季在中山站附近冰盖获取的湍流观测资料,应用空气动力学方法和涡动相关法计算分析了中山站至Dome A断面上近地层各种湍流参数(感热通量,潜热通量,湍流温度、湿度和速度尺度,地表粗糙度,大气稳定度及动量输送系数)的季节变化、日变...     

Extinction of Beamed Gamma-ray Burst Afterglows in a Dense Circumstellar Cloud

Broadband afterglow observations provide a probe of the density structure of the circumburst medium. In the spreading jet model, prompt and intense X-ray/UV radiation from the reverse shock may destroy and clear the dust in the circumburst cloud out to about 30 pc within the initial solid angle of the jet. Asthe jet expands significantly, optical radiation from the high-latitude part of the jet may suffer extinction by dust outside the initial solid angle, while radiation from the part within the initial solid angle can be observed without extinction. In previous studies, it is usually assumed that the extinction is complete. We calculate the extinction effect by taking the optical depth into account. Our numerical results showthat a break appears in the light curve of optical afterglow but it extends over a factor of ～ 80 in time rather than a factor of ～ 10 in time for the case of strong dust extinction and a factor of ～ 60 in time for the case without dust extinction. These results may provide a way to judge how large the number density of the circumburst cloud is. Finally, we carry out a detailed modeling for the afterglow of GRB 000926. Our model can provide a good fit to the multi-color observations of this event.     

A Detailed Study on the Equal Arrival Time Surface Effect in Gamma-Ray Burst Afterglows

Due to the relativistic motion of gamma-ray burst remnant and its deceleration in the circumburst medium, the equal arrival time surfaces at any moment are not spherical, rather, they are distorted ellipsoids. This will leave some imprints in the afterglows. We study the effect of equal arrival time surfaces numerically for various circumstances, i.e., isotropic fireballs, collimated jets, density jumps and energy injection events. For each case, a direct comparison is made between including and not including the effect. For isotropic fireballs and jets viewed on axis, the effect slightly hardens the spectra and postpones the peak time of the afterglows, but does not change the shapes of the spectra and light curves significantly. In the cases of a density jump or an energy injection, the effect smears out the variations in the afterglows markedly.     

The effect of spall on Lg waves

Introduction The Lg phase plays a central role in nuclear test detection, discrimination, and yield estima-tion because of its stability in propagation, but the excitation mechanisms of Lg phase are not fully understood. Regional Lg is a short-period guided wave composed mainly of a sequence of multi-ply reflected post-critical S waves trapped in the crustal wave guide. Several studies carried out recently (Gupta et al, 1992; Patton and Taylor, 1995; Gupta et al, 1997; Wallace, 1991) have …     

长湖浮游动物群落结构及其与环境因子的关系

为研究长湖浮游动物群落结构及其与环境因子间的关系,于2012年4月至2013年1月进行了4次调查采样。共鉴定出浮游动物67种(不包括原生动物),以轮虫种类为主(42种),其丰度与生物量均占据较大优势。浮游动物丰度的季节性差异显著,夏季最高(4412ind./L),冬季最低(831ind./L)。季节间的物种更替率大于59%,但优势种种类的季节变化不明显。优势种共8种,均为轮虫,萼花臂尾轮虫(Brachiouns calyciflorus)、针簇多枝轮虫(Polyarthra trigla Ehrenberg)是四个季节均出现的优势种,P.trigla Ehrenberg的优势度与出现频率均是各个季节的最大值,各季节这两种优势种的丰度和在总丰度的占比均超过59.13%。依据Shannon指数、Pielou指数、Margalef指数评价长湖水体处于中度污染,肥度指数评价长湖处于富营养状态。相关性分析、多元逐步回归方程、冗余分析的结果显示:水温是影响长湖浮游动物群落结构季节变化的关键因子;浮游植物表征含量chl a也是影响长湖浮游动物群落结构的关键因子,总氮、总磷通过影响浮游植物的群落结构间接地影响浮游动物的组成;能耐受较高p H的B.calyciflorus在长湖碱性水体中有较好的适应性;夏季马洪台区较低的溶解氧一定程度上限制了该区域轮虫的生长,总悬浮物通过降低溶解氧对浮游动物产生间接作用;化学需氧量对P.trigla Ehrenberg、螺形龟甲轮虫(Keratella cochlearis)等耐污种的影响较大,并对浮游动物的丰度产生正向作用。     

原生高砷地下水的类型、化学特征及成因

由于分布广、危害大,原生高砷地下水严重威胁全球内数亿居民的身体健康。研究原生高砷地下水的分布、化学特征及成因有助于进一步理解地下水中砷的迁移转化规律,并确保高砷区地下水的可持续利用。在查阅大量文献资料的基础上,结合近10年的高砷地下水研究经验,把原生高砷地下水分为还原性中性高砷地下水（Ⅰ 1型）和还原性弱碱性高砷地下水（Ⅰ 2型）、氧化性弱碱性高砷地下水（Ⅱ型）和氧化性弱酸性高砷地下水（Ⅲ型）。Ⅰ 1型高砷地下水主要分布于河流三角洲地区,Ⅰ 2型分布于干旱半干旱封闭内陆盆地,Ⅱ型主要分布于干旱半干旱平原盆地,Ⅲ型主要分布于富含黄铁矿或硫化物矿物的基岩地区。Ⅰ 1型高砷地下水处于还原环境,pH呈中性,Fe/Mn氧化物矿物的还原性溶解是造成As富集的主要原因。Ⅰ 2型高砷地下水处于还原环境,pH呈弱碱性,除了Fe/Mn氧化物矿物的还原性溶解外,As的解吸附是含水层中砷释放的重要原因。Ⅱ型高砷地下水处于氧化弱氧化环境,pH呈弱碱性,As的解吸附是含水层中砷释放的主要原因。Ⅲ型高砷地下水处于氧化环境,pH呈弱酸性,黄铁矿及其他硫化物矿物的氧化溶解导致了含水层中砷的释放。对于Ⅰ 2型高砷地下水,需要深入研究Fe/Mn氧化物矿物的还原性溶解以及As的解吸附对地下水砷富集的相对贡献量。     

Effect of salt concentration on desiccation cracking behavior of GMZ bentonite

Bentonite has been proposed for use as an engineering barrier and buffer in nuclear waste repositories and has been used frequently in municipal waste landfills. The cracking behavior and deformation properties of this material can be influenced by the chemistry of pore water. In the present work, the influence of salt concentration on the desiccation cracking behavior of GMZ bentonite was investigated with laboratory experiments. Image processing techniques and SEM tests were performed on the specimens which had undergone the desiccation testing in order to analyze the cracking mechanisms. Results show that the water evaporation process can be identified by a steady rate stage, a falling rate stage and a residual stage. The water evaporation rate is strongly affected by the salt concentration of the pore water; higher salt concentrations result in lower evaporation rates; the final water content is strongly impacted by a high initial salinity; otherwise the water contents are very similar for the residual stage. During desiccating, most of cracks appeared at the steady evaporation stage. The cracking morphology and patterns were greatly affected by the salt concentration of the pore water; and larger crack lengths and lower crack densities were obtained as the initial salinity was increased.