A 20.1 W Solid-State Laser Pumped by 887 nm with High Efficiency and TEM00 Mode

High efficiency, TEM00 mode, high repetition rate laser pumped by 887 nm is reported. 20.1 W output laser emitting at 1064 nm is achieved in a 0.3 at % Nd-doped Nd:YVO4, which absorbs pumping light of 30.7 W at 887 nm. The opto-optic efficiency and the slope efficiency are 65.5 and 88.5%, respectively. The stable Q-switching operation worked well at 100 kHz and the beam quality is near diffraction-limit with M-2 factor measured as M-2 approximate to 1.2. And the pulse waveform is analyzed in this paper.

Effects of Yb ion concentration on the spectral properties of lead silica glasses

The spectral properties in different concentration of Yb ions (0.5-5 mol%)-doped silica glasses are explored in this paper. The glasses are prepared by traditional melting method. The absorption spectra and the fluorescent lifetime (tau(f)) are measured at room temperature and low temperature (18 K). The stimulated cross-section (sigma(emi)) and potential laser properties (beta(min), I-sat, I-min) are calculated based on the absorption spectra. The absorption cross-section (sigma(abs)) are in the range 1.08 x 10(-20) - 1.18 x 10(-20) cm(2) in different glasses, the fluorescence lifetime (tau(f)) change from 1.9 to 1.2 ms with the increase of Yb3+ concentration. The potential laser properties indicate that lead silica glass is a good host for highly Yb ion doping glass. (c) 2005 Elsevier B.V. All rights reserved.

南极中山站、长城站附近18个湖泊生态学特征的逐步判别分析

南极中山站、长城站附近１８个湖泊生态学特征的逐步判别分析蔡庆华，王洪铸，梁彦龄（中国科学院水生生物研究所，武汉４３００７２）关键词南极，湖泊，生态学特征，逐步判别分析，拉斯曼丘陵，乔治王岛ＳＴＥＰＷＩＳＥＤＩＳＣＲＩＭＩＮＡＮＴＡＮＡＬＹＳＩＳＦＯＲ...

Narrow-beam divergence 1.55μm laser diodes with integrated self-aligned spotsize conVerter

This paper describes the high performance of narrow-beam divergence spot size converter (SSC) integrated separately confined heterostructure (SCH) LD. The upper optical confinement layer (OCL) and the butt-coupled tapered thickness waveguide were regrown simultaneously, which not only offered the separated optimization of the active region and the integrated spotsize converter, but also reduced the difficulty of the butt-joint selective regrowth. The threshold current was as low as 5.4 mA, the output power at 55 mA was 10.1 mW, the vertical and horizontal far field divergence angles were as low as 9°and 15°, and the 1-dB misalignment tolerances were 3.6 and 3.4μm, respectively.

LFX-20型逆燃式医疗废物焚烧炉二恶英实测分析

概述我国目前医疗废物焚烧处置中的主要炉型,着重介绍LFX-20型逆燃式焚烧炉焚烧处置医疗废物的实际运行工况。在1燃室、2燃室平均温度分别为869.5℃和898.7℃条件下,对医疗废物焚烧烟气进行检测。各项常规指标均低于国标限值,二恶英检测中其质量浓度实测值为15ng/m3,相应毒性当量为0.46ngTEQ/m3,同时对医疗废物焚烧后产生烟气中二恶英和灰渣的检测结果进行了分析,焚烧后底渣体积约为焚烧前医疗废物体积的1/10,重量为原来的12%～18%,飞灰热灼减率为34.6%,并给出分析结果。

Direct numerical simulation of hypersonic boundary layer transition over a blunt cone with a small angle of attack

The direct numerical simulation of boundary layer transition over a 5° half-cone-angle blunt cone is performed. The free-stream Mach number is 6 and the angle of attack is 1°. Random wall blow-and-suction perturbations are used to trigger the transition. Different from the authors’ previous work [Li et al., AIAA J. 46, 2899(2008)], the whole boundary layer flow over the cone is simulated (while in the author’s previous work, only two 45° regions around the leeward and the windward sections are simulated). The transition location on the cone surface is determined through the rapid increase in skin fraction coefficient (Cf). The transition line on the cone surface shows a nonmonotonic curve and the transition is delayed in the range of 0° ≤ θ ≤ 30° (θ = 0° is the leeward section). The mechanism of the delayed transition is studied by using joint frequency spectrum analysis and linear stability theory (LST). It is shown that the growth rates of unstable waves of the second mode are suppressed in the range of 20° ≤ θ ≤ 30°, which leads to the delayed transition location. Very low frequency waves VLFWs� are found in the time series recorded just before the transition location, and the periodic times of VLFWs are about one order larger than those of ordinary Mack second mode waves. Band-pass filter is used to analyze the low frequency waves, and they are deemed as the effect of large scale nonlinear perturbations triggered by LST waves when they are strong enough.The direct numerical simulation of boundary layer transition over a 5° half-cone-angle blunt cone is performed. The free-stream Mach number is 6 and the angle of attack is 1°. Random wall blow-and-suction perturbations are used to trigger the transition. Different from the authors’ previous work [ Li et al., AIAA J. 46, 2899 (2008) ], the whole boundary layer flow over the cone is simulated (while in the author’s previous work, only two 45° regions around the leeward and the windward sections are simulated). The transition location on the cone surface is determined through the rapid increase in skin fraction coefficient (Cf). The transition line on the cone surface shows a nonmonotonic curve and the transition is delayed in the range of 20° ≤ θ ≤ 30° (θ = 0° is the leeward section). The mechanism of the delayed transition is studied by using joint frequency spectrum analysis and linear stability theory (LST). It is shown that the growth rates of unstable waves of the second mode are suppressed in the range of 20° ≤ θ ≤ 30°, which leads to the delayed transition location. Very low frequency waves (VLFWs) are found in the time series recorded just before the transition location, and the periodic times of VLFWs are about one order larger than those of ordinary Mack second mode waves. Band-pass filter is used to analyze the low frequency waves, and they are deemed as the effect of large scale nonlinear perturbations triggered by LST waves when they are strong enough.

Optical transmission larger than 1 (T > 1) through ZnS-SiO2/AgOx/ZnS-SiO2 sandwiched thin films

Optical transmission through flat media should be smaller than 1. However, we have observed optical transmission up to T=1.18. The samples were ZnS-SiO2/AgOx/ZnS-SiO2 sandwiched thin films on glass substrate. The supertransmission could only be observed in the near field. We attribute the supertransmission to the lateral propagation relayed by the laser activated and decomposed Ag nanoparticles. (c) 2006 American Institute of Physics.

百合科黄精族的系统学研究

黄精族隶属于广义的百合科，通过对其研究历史的回顾，指出了它目前存在的问题，即(1)族的概念和范围不清、(2)属间的界限模糊、(3)族内各属的系统排列不明确．针对这些问题，本文从形态、解剖、胚胎、孢粉和细胞方面对族内各类群进行了野外调查和一些实验工作，本此基础上，并结合前人的工作，对黄精族的系统发育进行了探讨． 一, 形态本文通过黄精族各属大量标本，尤其是国产类群标本的认真研究，并结合6个多月的野外调查资料，分析了本族植物21个形态性状及其状态在属间和属内的分布，指出了一些性状的稳定性及其系统学价值， 二，解剖本文对黄精族5属17个种的茎、根状茎及子房进行了解剖学观察，同时对7属41种植物的叶表皮进行光镜观察，并对5属12种的叶表皮进行扫描电镜的观察，结果表明：(1)七筋姑属花葶的维管柱缺乏纤维鞘，这和本族其它类群不同．(2)扭柄花属、黄精属、竹根七属和鹿药属植物子房中具草酸盐针晶，而七筋姑属和万寿草属未发现这种晶体．(3)本族植物的气孔器均为无规则型，但邻近细胞及其周壁的形状在不同类群中是不同的，据此我们将本族叶表皮划分为七个类型，并认为叶表皮邻近细胞呈多边形、周壁直是黄精族叶表皮最基本的形式． 三，胚胎本文对黄精族3属4种植物以及铃兰(Convallaria majalis)进行了胚胎学研究，其中小玉竹(Polygonatum humile)和铃兰得到了完整的胚胎学资料，实验结果显示(1)黄精族植物小孢子发生过程中胞质分裂均为连续型，胚乳发育为核型;(2)小玉竹的胚囊发育方式为葱型，鹿药(Smilacina japonica)为英地百合型．万寿竹(Disporum cantoniense)和长蕊万寿竹(D. bodinicri)为蓼型，铃兰为葱型或英地百合型;(3)周缘细胞的有或无在小玉竹，鹿药和铃兰中是不稳定的． 四，孢粉本文对6属42种植物花粉进行了扫描电镜观察，结果表明(1)萌发孔的类型和数目在本族中不稳定，系统价值不大;(2)花粉外壁纹饰比较稳定，是一个十分重要的分类学性状．我们将黄精族植物的花粉外壁纹饰划分为9种类型．并认为孔穴型是一种原始类型，其它类型是由它演化而成， 五，细胞在前人工作的基础上，通过与其它性状的综合分析，本文认为黄精族植物有五种原始染色体基数：七筋姑属x=7;万寿竹属和扭柄花属x=8;黄精属x＝9：鹿药属和舞鹤草属x＝ 18;竹根七属x=20． 在上述实验结果的基础上，结合前人的工作，对黄精族的各种性状进行了分析，本文得出如下结论： 1．包括万寿竹属、扭柄花属、七筋姑属、黄精属、竹根七属、鹿药属和舞鹤草属的黄精族是一个单系类群． 2．本文赞同Dahlgren et al．(1985)，Tahktajan (1987)对黄精族系统位置的处理，即它与铃兰族，蜘蛛抱蛋族和沿阶草族关系较近，且共同组成铃兰科．相比之下，黄精族是该科中比较原始的一个族. 3．本文在性状分析的基础上，总结出20个比较稳定、系统价值较大的性状，并指出了它们的演化趋势;同时总结出黄精族原始类群应具有如下特征：(1).具细线形根状茎;(2).地上茎具分枝;(3).叶茎生;(4).具腋生的圆锥或总状花序;(5).花为三基数，花被片离生;(6).花被片具多条开放型脉;(7) .胚珠多数;(8).胚囊发育为单孢子型;(9).厚珠心胚珠;(10) .花粉外壁具覆盖层． 4．本文认为黄精族植物可分为三支：一是以染色体基数x＝9及其衍生的类群，包括黄精属，竹根七属、鹿药属和舞鹤草属;二是以x=8为基数的一支，它包括万寿竹属和扭柄花属;三是七筋姑属单独形成的一支，它的染色体基数x＝7．同时认为万寿竹属是本族比较原始的一个类群． 5．本文认为东亚北方是黄精族植物起源地． 6．本文赞同汤彦承(1978．见汪发缵、唐进1978)对卵叶扭柄花(Streptopus ovalis (Ohwi) Wang et Y.C．Tang)的分类学处理，而不赞同汪发缵、唐进(1983)把金佛山鹿药(Smilacina jinfoshanica Wang et Tang)从鹿药属转隶至黄精属的观点． 7．本文认为鹿药属和舞鹤草属亲缘关系较近，但区别特征明显，从而不赞同LaFrankie (1986),李恒(1990)将二者合并的观点。

东灵山森林生态系统若干水分问题的研究

东灵山地区年均降水量659.7mm，单次降水以雨量小、雨强低的降水为主。水汽压（年均17.7mb）、相对湿度（年均66％）的季节变化呈现生长季高、冬季低的趋势。年均蒸发量1019.5mm;气温、风速、日照时间和水压与月蒸发量和日蒸量相关显著;气温、日照时间和水压分别在11-6月、7－8月和9－10月为决定蒸发量的首要因子。枯枝落叶层、土壤层湿度主要受前十日降水量和坡向影响。 植物体含水量生长季节较高，冬季较低;含水量随径级的增大而降低。六个灌木树种的平均含水量大小顺序为：毛榛（48.62%）最高荆条（36.32%）最低;七个乔木树种水分含量为油松，56.14%;蒙椴，54.19%;华北落叶松，52.91%;五角枫，43.64%;辽东栎，41.87%;棘皮桦，41.13%;大叶白腊，37.79%。几种植被类型的储水量为：辽东栎林，82.08mm;华北落叶松林，47.35mm;混交林，34.60mm;油松林，31.33mm;灌丛，12.40mm。各树种叶片日最低水势的季节均值为：辽东栎，-16.1bar;五角枫，-15.8bar;大叶白腊，-15.1bar;糠椴，-13.4bar;棘皮桦，-12.3bar;蒙椴，-12.2bar。叶片水势的日间变化均呈一“V”形曲线;光照在叶片水势的日间变化中起着决定性作用。 96年各树种平均单株树干茎流量为辽东栎，30.3mm(4.19%);华北落叶松，16.1mm(2.22%);油松，8.9mm(1.23%);棘皮桦，2.9mm(0.40%)。两个生长季各林分冠层的水量平衡为：辽东栎林，树干流茎量101.87mm(9.18%)，穿透降水量823.08mm(74.15%)，截留量185.05mm(16.67%);华北落叶松林，树干径流量66.88mm(6.03%)，穿透降水量836.92mm(75.40%)，截留量206.20mm(18.58);混交林，树干径流量50.13(4.52%)，穿透降水量846.78mm(76.29%)，截留量212.20mm(19.12%);油松林，树干径流量33.90mm(3.05%)，穿透降水量934.88mm(84.22%)，截留量141.22mm(12.72%)。多元回归分析表明，树干流茎量S与降水量P和前24小时降水量P_1呈显著正相关关系;穿透降水量T与降水量P和最大雨强M正相关显著。附加截留量与降水时间成正比。 枯枝落叶层的生物量为：油松林，25.56t/hm~2;华北落叶松林20.01t/hm~2;辽东栎林，8.31t/hm~2;混交林，7.98t/hm~2。枯枝落叶层的平均实际持水量和有效持水量均以油松林最大，其次是华北落叶松林，而混交林和辽东栎林较低;枯枝落叶层的实际持水量和有效持水量的季节变化分别与前十日降水量P10成正相关和负相关关系。枯枝落叶层的截留量为油松林＞华北落叶松林＞辽东栎林＞混交林;油松林（145.632mm和90.800mm）混交林(61.816mm和54.504mm)。油松林、辽东栎林、混交林和华北落叶松林去除枯枝落叶层后，土壤入渗量比对照平均降低100mm以上;表层土壤含水量分别比对照土壤下降了6.26、18.26、15.06和15.07个百分点。地表径流量分别增加了，辽东栎林34.299mm(603%)和15.816mm(525%);油松林14.593mm(732%)和10.584mm(1321%);混交林12.004mm(181%)和7.275mm(364%);华北落叶松林3.555mm(118%)，3.275mm(229%)。96年生长季，各土壤流失量分别增加了：油松林172.751t/hm~2(124倍);辽东栎林836.500t/hm~2(119倍);混交林172.499t/hm~2(47倍);华北落叶松林11.557t/hm~2(11倍)。表层土壤容重分别增加了：油松林15.0%和20.6%，辽东栎林18.4%和28.2%，混交林11.5%和38.5%，华北落叶松林4.3%和17.1%。 0-60cm深度土壤容重平均值的大小顺序为：草地>灌丛>辽东栎林>油松林>混交林>华北落叶松林;而土壤孔隙度的大小顺序为华北落叶松林>混交林>油松林>辽东栎林>灌丛>草地。两个生长季为土壤实际储水量的均值：油松林，124.45mm，78.62mm;辽东栎林，131.23mm，87.72mm;混交林，180.41mm，113.90mm;华北落叶松林，165.53mm，127.95mm;灌丛，172.50mm，89.81mm;草地，152.92mm，89.59 mm分别比干旱年份97年高出45.83mm、43.51mm、51.63mm、37.58mm、82.69mm和63.33mm。两个生长季的地表径流量为草地，30.930mm(2.79%);灌丛，16.321mm(147%);油松林，2.911mm(0.26%);辽东栎林，8.703mm(0.78%);混交林，8.625mm(0.78%);华北落叶松林，4.447mm(0.40%)。油松林、混交林和华北落叶松林地表径流量与降水量P(mm)和最大雨强(mm/h)正相关显著;而辽东栎林、灌丛和草地的地表径流量则与降水量P(mm)、平均雨强Q(mm/hr)和最大雨强M(mm/hr)三者之间呈显著正相关关系。与草地相比(1220.093kg/hm~2，100％)，灌丛、辽东栎林、混交林、油松林和华北落叶松林96年生长季的土壤流失量分别降低了85.05%、94.26%、96.99%、98.86和99.14%。 降水量是影响小流域径流量时间变化的主要因素;南沟和马牙石沟96年的径流量分别是97年的8.19倍和7.87倍，而径流深(46.25mm，52.75mm)分别比97年(5.65mm,6.70mm)高出40.60mm和46.05mm。两个小流域由于面积的差异而使南沟两年的径流量分别比马牙石沟高出2773.136m~3(13.15%)和235.434m~3(8.79%)。96年和97年马牙石沟径流深比南沟高出6.5mm(14.05%)和1.05mm(18.58%)。在地处大陆性季风气候区的东灵山地区，用0.010m~3/min/km~2/hr能较好地分割小流域的洪峰和基流。在五次暴雨水文曲线中，马牙石沟的快速径流量分别比南沟高出25.00%到143.33%。五次洪水水文响应R的平均值南沟为0.218%，马牙石沟为0.404%;与海洋性气候地区相比，东灵山地区小流域的R值要低一到两个数量级。马牙石沟洪峰流量Qp的平均值为418.772L/min要比南沟(281.191L/min)大48.9%。东灵山地区小流域的洪水径流过程可分为三种类型。

紫茎泽兰种群补充特征

外来种紫茎泽兰 (Eupatorium adenophorum Spreng.) 对我国西南地区生态系统的危害已长达50~60年之久，我国于20世纪70年代开展紫茎泽兰的研究，但目前仍然没有能力将其限制在一个可控范围之内，随着我国对生物多样性重要性认识的加深，对于紫茎泽兰的研究也越来越深入。本文以四川攀枝花受入侵生态系统为例，通过对该地区植被、土壤种子库以及当地紫茎泽兰无性繁殖和种子萌发特征开展研究，分析受入侵生态系统的特征，结合紫茎泽兰种群补充特征，揭示紫茎泽兰入侵机制，探索管理受害生态系统的方法。 所选实验点为紫茎泽兰危害严重的地带，群落中紫茎泽兰为优势种，伴生种灌木18种，草本植物65种，草本层以紫茎泽兰最为昌盛，种群构成为1～4年生植株与其荫庇下大量的实生幼苗，Drude多度极大，频度达100%。紫茎泽兰与灌木重要值之间极显著负相关 (P<0.01) ，与其他草本重要值之间极显著负相关 (P<0.01) ，灌木与其他草本重要值间的相关性不显著 (P>0.05) 。说明紫茎泽兰的生长与灌木或草本间存在微妙的此消彼长的关联，充分显示了紫茎泽兰与当地物种间的竞争事实。 紫茎泽兰种子雨前的种子库为所研究地区绝大部分物种的长久性土壤种子库，本地区种子库的组成物种共有13种，包括灌木和草本。紫茎泽兰占整个种子库储量的61.3%，在长久种子库中占有明显的优势;种子库与植被间相似度为0.31，虽然种子库中物种均为植被的组成成分，但是植被中绝大多数物种种子未检测出，种子库中出现的物种与该物种本身的生理生态特性密切相关。种子雨是种子库的来源，紫茎泽兰种子雨前表层种子储量只占种子雨后的7.4%，中下层储量占33.8%，共占41.2%，即每年仅58.8%的种子在当年雨季萌发，剩余的在土壤中保持休眠状态。依 目前的研究结果，本地植被仅靠自然恢复的可能性不大。 紫茎泽兰种子最适发芽温度为25℃;储藏1.5 a后的种子萌发率有所下降，25℃下萌发率由77%下降为66%;紫茎泽兰种子有良好的休眠机制，对生境的干扰可以促进紫茎泽兰长久土壤种子库的形成，为紫茎泽兰种群补充奠定了基础。稀疏的植被有利于紫茎泽兰种子萌发及幼苗建植，对原生植被的破坏则促进了紫茎泽兰实生苗的补充。因而保护原始生境、减少对原生态系统的破坏，是减少和抑制紫茎泽兰种群补充的有效途径。 紫茎泽兰 (克隆) 离体无性繁殖的部位为根颈部分，其他离体部分没有无性繁殖能力或很弱;灌丛和路域生境下的离体部分在给予相同培养条件下，克隆繁殖效益有差别，灌丛生境萌芽较早，而主茎和叶生长速度较慢。拔除干扰对于紫茎泽兰萌生新枝具有刺激作用，对紫茎泽兰植株上部的割取类似于给它提供更新复壮的机会，因此在紫茎泽兰防治过程中一定要注意将其拔除干净，以防后患。