182 resultados para ±0.3


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于2010-11-23批量导入

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国家自然科学基金

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Red shifts of emission wavelength of self-organized In(Cla)As/GaAs quantum dots (QDs) covered by 3 nm thick InxGa1-xAs layer with three different In mole fractions (x = 0.1, 0.2 and 0.3, respectively) have been observed. Transmission electron microscopy images demonstrate that the stress along growth direction in the InAs dots was reduced due to introducing the InxGa1-xAs (x = 0.1, 0.2 and 0.3) covering layer instead of GaAs layer. Atomic force microscopy pictures show a smoother surface of InAs islands covered by an In0.2Ga0.8As layer. It is explained by the calculations that the redshifts of the photoluminescence (PL) spectra from the QDs covered by the InxGa1-xAs (x greater than or equal to 0.1) layers were mainly due to the reducing of the strain other than the InAs/GaAs intermixing in the InAs QDs. The temperature dependent PL spectra further confirm that the InGaAs covering layer can effectively suppress the temperature sensitivity of PL emissions. 1.3 mum emission wavelength with a very narrow linewidth of 19.2 mcV at room temperature has been obtained successfully from In,In0.5Ga0.5As/GaAs self-assembled QDs covered by a 3-nm In0.2Ga0.2As strain reducing layer. (C) 2001 Elsevier Science B.V. All rights reserved.

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For (Ti1-xVx)(2)Ni (x = 0.05,0.1,0.15,0.2 and 0.3) ribbons, synthesized by arc-melting and subsequent melt-spinning techniques, an icosahedral quasicrystalline phase was present, either in the amorphous matrix or together with the stable Ti2Ni-type phase. With increasing x values, the maximum discharge capacity of the alloy electrodes increased until reached 271.3 mAh/g when x = 0.3. The cycling capacity retention rates for these electrodes were approximately 80% after a preliminary test of 30 consecutive cycles of charging and discharging.

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Mg-5Al-0.3Mn-xCe (x = 0-3, wt.%) alloys were prepared by metal mould casting method. The microstructures and mechanical properties were investigated. The results revealed that the main phases of as-cast Mg-5Al-0.3Mn alloy consist of alpha-Mg matrix and beta-Mg17Al12 phase. With the addition of Ce element, Al11Ce3 precipitates were formed and mainly aggregated along the grain boundaries. The amount of the Al11Ce3 precipitates increased with increasing addition of Ce, but the amount of beta-Mg17Al12 phase decreased. The highest tensile strength was obtained in Mg-5Al-0.3Mn-1.5Ce alloy. The ultimate tensile strength (UTS), yield strength (YS) and elongation at room temperature are 203 MPa, 88 MPa and 20%, separately.

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采用XRD、FESEM-EDS、ICP及EIS等方法研究了Ti0.17Zr0.08V0.34Nb0.01Cr0.1Ni0.3氢化物电极合金微观结构和电化学性能。X射线衍射分析表明:该合金由体心立方结构(bcc)的V基固溶体主相和少量六方结构的C14型Laves相组成;FESEM及EDS分析表明:V基固溶体主相形成树枝晶,C14型Laves相呈网格状围绕着树枝晶的晶界,元素在两相中的分布呈现镜像关系。电化学性能测试结果表明:该合金的氢化物电极在303 ̄343K较宽的温度区间内,表现出较高的电化学容量,在303K和343K时,电化学容量分别为337.0mAh·g-1和327.9mAh·g-1。在303K循环100周后,容量为282.7mAh·g-1。ICP分析结果表明,氢化物电极在充放电循环过程中,V及Zr元素向KOH电解质中的溶出较为严重。EIS研究表明,金属氢化物电极表面电化学反应的电荷转移电阻(RT)随循环次数的增加而增加,相应的交换电流密度则随循环次数的增加而降低。氢化物电极循环过程中RT的增大以及V和Zr元素的溶解,可能是导致电极容量衰减的主要原因。

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The chemical bond parameters, that is, bond covalency, bond susceptibility, and macroscopic linear susceptibility of La1-xCaxCrO3 (x = 0.0, 0.1, 0.2, 0.3) has been calculated using a semiempirical method. This method is the generalization of the dielectric description theory proposed by Phillips, Van Vechten, Levine, and Tanaka (PVLT). In the calculation of bond valence, two schemes were adopted. One is the bond valence sums (BVS) scheme, and the other is the equal-valence scheme. Both schemes suggest that for the title compounds bond covalency and bond susceptibility are mainly influenced by bond valence and are insensitive to the Ca doping level or structural change. Larger bond valences usually result in higher bond covalency and bond susceptibility. The macroscopic linear susceptibility increases (only slightly for BVS scheme) with the increasing Ca doping level. (C) 1999 John Wiley & Sons, Inc.

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利用YJ-3000t和JL-3600t多顶砧压力机,以哀牢山造山带南部红河县大白能—乐育剖面上的天然块状斜长角闪岩为初始样品,在950℃、1.0~3.5GPa、恒温20~300h条件下进行了两个系列的斜长角闪岩块状样品脱水部分熔融实验:(1)保持温度T=950℃,加热时间t=100h不变,改变压力(1.0~3.5GPa)的实验;(2)保持温度T=950℃,压力p=3.0GPa不变,改变加热时间(20~300h)的实验。结果表明,1.0~3.5GPa、950℃、恒温100h的条件下,随压力升高,斜长角闪岩中依次生成了单斜辉石+石榴石+熔体的矿物组合(1.0~1.5GPa)和单斜辉石+石榴石+熔体+硬玉+SiO2矿物+蓝晶石(2.0~3.5GPa)的矿物组合。3.0GPa、950℃条件下,随加热时间增加,实验产物中依次生成了单斜辉石+石榴石+熔体+硬玉+SiO2矿物+蓝晶石的矿物组合(20~100h)和单斜辉石+石榴石+熔体的矿物组合(150~300h)。斜长角闪岩的原岩结构决定了实验产物中新生矿物和熔体的分布。依据实验产物的矿物组合和新生矿物的分布特征,讨论了950℃、1.0~3.5GPa、恒温(20~300h)条件下,斜长角闪岩部分熔融过程的结构变化、变质反应以及石榴石冠状体的成因。

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Mg-8Gd-0.6Zr-xNd-yY (mass%) alloys which containing different Nd:Y mass ratio of 3:0, 2:1, 1:2 and 0:3 with a constant x + y = 3 were prepared by metal mould casting method, and the microstructure, aging behaviour and tensile properties have been investigated. The fibrous eutectic areas along the boundaries enlarge clearly in the as-cast alloys containing Y element, and the fine grain boundaries and dispersed precipitation are observed in the aged alloys. The Mg-8Gd-0.6Zr-2Nd-Y alloy exhibits notably age-hardening behaviour and the highest mechanical property. The ultimate tensile strength and yield strength of Mg-8Gd-0.6Zr-2Nd-Y alloy in the peak aged hardness are 293 and 221 MPa at room temperature, 248 and 191 MPa at 230 degrees C. The improvement of age-hardening response and tensile properties is mainly attributed to the quadrate-like stable Mg5RE precipitate, which forms readily and orderly in aged Mg-8Gd-0.6Zr-2Nd-Y alloy.

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We demonstrate passive Q-switching of short-length double-clad Tm3+-doped silica fiber lasers near 2 mu m pumped by a laser diode array (LDA) at 790 nm. Polycrystalline Cr2+:ZnSe microchips with thickness from 0.3 to 1 mm are adopted as the Q-switching elements. Pulse duration of 120 ns, pulse energy over 14 mu] and repetition rate of 53 kHz are obtained from a 5-cm long fiber laser. As high as 530 kHz repetition rate is achieved from a 50-cm long fiber laser at similar to 10-W pump power. The performance of the Q-switched fiber lasers as a function of fiber length is also analyzed. (c) 2008 Elsevier B.V. All rights reserved.

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A series of tellurite glasses of composition, 75TeO(2)-20ZnO-(5 - x)La2O3-xEr(2)O(3) (x = 0.05, 0.1, 0.3, 0.6, 1.0, 2.0, and 3.0 mol%) with different hydroxl content were prepared. The effect of Er3+ and OH- groups concentration on the emission properties of Er3+: I-4(13/2) -> I-4(15/2) transition in tellurite glasses was investigated. The constant KOH-Er for Er3+ in tellurite glasses, which represents the strength of interaction between Er3+ and OH- groups in the case of energy migration, was about 14 x 10(-19) cm(4) s(-1). The interaction parameter C-Er,C-Er for the migration rate of Er3+ : 4I(13/2) -> I-4(13/2) transition in tellurite glass was 46 x 10(-40) cm(2), which indicates that concentration quenching in Er3+-doped modified tellurite glass for a given Er3+ concentration is much stronger than in silicate and phosphate glasses. (c) 2007 Elsevier B.V. All rights reserved.

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通量测量点的能量收支总是表现出不平衡,即使在地势平坦、植被分布均一、稀疏植被下垫面的情况下也有约30%的能量失衡状况。能量平衡闭合 (EBC) 问题在验证涡度相关系统质量方面,得到了广泛的关注。实验在内蒙古草原3个地点,通过涡度相关系统附近移动能量平衡系统的测定手段,采用能量平衡余项法和最小二乘 (OLS) 线性回归法,研究了土壤热通量、净辐射及可供能量空间变异对能量平衡闭合的影响。 结果显示,EBC 在三个研究点的平均余项为8~19 W m-2,OLS 斜率为0.83~0.96。EBC 在土壤湿润情况的站点要高于干旱站点。 土壤热通量的空间变异三站点平均为白天48 W m-2 (占同时间 Rn 的13%),夜间15 W m-2 (34%),平均29 W m-2 (24%)。通过8个工作站的测量,这个变异会造成9% (从0.93到1.01) 的 OLS 斜率差别。夜间的能量平衡不闭合可以由土壤热通量的空间变异解释。如果在本研究的的三个草原站点上忽略了土壤热通量,则会造成较大的余项 (峰值时110 W m-2) 产生,从而使 OLS 斜率增大23%。特别是通量板埋置在地面以下30 mm处时,上层的土壤热储部分占到全部土壤热通量的50%,这不仅影响到 EBC 的大小,更起到调节土壤热通量与“真实的波形” 相一致的作用。如果该部分热储被忽略掉,EBC 余项会增加60 W m-2,OLS 斜率也会变化 (减少) 9%。用大尺度多点测量与涡度塔附近的小尺度测定相比较,后者表现出稍高的闭合率,即 OLS 斜率增加4%。 相对于土壤热通量,净辐射的空间变异较小,三站点平均为白天17 W m-2 (5%),夜间7 W m-2 (13%),平均 12 W m-2 (5%)。可以引起3% (从0.88到0.91) 的 OLS 斜率差异。研究结果还表明,风速校正应该在 Q7.1 净辐射仪中应用,校正后的结果与 CNR1 的结果在白天有吻合较好,但在其它时段仍有较大差异,特别是在夜间,风速校正基本不起作用,使得两种仪器间差异达20 W m-2。比较表明,风速校正可以提高白天 Rn 的6%,仅降低夜间0.3%。因此,无论是用余项法还是用 OLS 线性回归法,在比较使用不同仪器的站点间的闭合状况时 (本研究的结果适用于草地 Q7.1 与 CNR1 间的比较),可以用9:00-15:00 h 时段的数据进行比较,这样可以避免因使用不同仪器的差异所造成的影响。用该时段的数据进行比较,仪器间的差异余项法小于6 W m-2,OLS 法小于3%。 受可供能量空间变异影响,三个站点平均 EBC 的不确定性为白天66 W m-2 (19%),夜间23 W m-2 (50%),平均42 W m-2 (36%);或者改变 OLS 斜率11%。用最大值和最小值来衡量,EBC 最大不确定性,正午时在站点 I、II 和 III 中分别为81,114和91 W m-2。故在探讨能量平衡和能量平衡闭合问题时,必须充分考虑到这种不确定性,否则会产生偏差,或者得出错误结论。 研究还表明,即使考虑到白天所有可供能量的最大不确定性,仍然不能使能量平衡闭合。中午 (12:00 h),站点 I,II 和 III 仍然有14±15,48±12和47±14 W m-2 的失衡不能够归因于可供能量的空间不确定性。因此,其它影响因素也需进行细致的探讨。 在两站点不同测量深度土壤热通量结果的差异性比较实验中,无论在站点 I 还是 III,均表现出一致的结论,即随通量板布置深度加深,其测量结果会越高,与浅层布置的相比,差别可高达150 W m-2。深层土壤热通量的计算仍是个难题,需进一步研究。 在不同植被结构对净辐射测定影响的实验中发现,随刈割强度增加,一天中大部分时间净辐射均减少。正午依次为413,395和388 W m-2。无论正午还是全天合计,重度刈割地点的净辐射均比不刈割对照处理少6%,而且,在整个生长季也少6%,约合40,000 W m-2。测量高度不同,不同处理间对测定结果影响不同:刈割处理中,由于下垫面较均一,结果相差不显著;而对照则表现出较高的差异,用两配对样本T检验表明差异达到极显著 (P<0.000,9:30-15:00 h data)。当使用不同新旧程度的 domes 时,对净辐射结果会产生明显的影响。新 domes 的测量结果白天明显高,晚上明显低,使用了11个月的旧 domes,峰值时,白天低估25 W m-2,晚上高估10 W m-2。说明该差异在进行能量平衡闭合计算时,不能忽略。而全用新的和全用旧的进行比较,晚上仅有2-3 W m-2差异。 考虑生态系统中非生物因子对干扰条件下生物多样性动态和功能的影响,有助于更精确地阐明生物多样性-稳定性功能的关系。为此,设计了一个单因子刈割实验——内蒙古地区一种广泛存在的土地利用方式。主要目的是研究不同强度刈割影响下,微气候变量特别是能量平衡各分量和群落结构的变化及二者的关系。连续4年刈割,占第一位的优势种明显由低矮半灌木冷蒿 (Artemisia frigida) 取代了高大丛生禾草克氏针茅 (Stipa kylovii)。重度刈割下,针茅的盖度、生物量和丛重,群落叶面积、绿色生物量、凋落物量和群落高度一致低于轻度刈割/不刈割处理。微气候由于群落特征的这些变化也呈规律性变化。与对照相比,重度刈割降低了生长季土壤含水量的47.5%,但中午和日均土壤表面温度分别增加了7.4和1.2 °C,并且增加地表下2 cm土壤温度日较差 (日最高与最低温度之差) 4.2 °C。刈割处理由于凋落物少、反射强而表现出较低的净辐射,但土壤热通量显著提高,表现为土层加热和冷却快。因此,重度刈割处理较对照降低了可供能量8%,约合52,000 W m-2 。不同刈割强度间来看,NPP 或 LAI 与土壤热通量和净辐射的比值 (G/Rn) 以及波文比 (H/LE) 间呈负相关。重度刈割处理感热通量显著提高,但潜热通量在处理间差异不显著,表明未刈割处理虽然冠层伸展大,但是并没有导致更大的水分亏缺。未刈割处理增加了抵抗物种改变的能力,而刈割处理在连续一年一割的第四年显著增加了物种数,可能与因刈割影响而导致的群落结构与微气候的改变有关。本研究表明,未刈割处理可以减轻高温干旱季节的高温和干旱胁迫,表现出对环境变化的高抵抗性。未刈割处理的凋落物层和较高的垂直结构所形成的遮荫,可以形成一个阻挡蒸发的篱笆,这是维持其水分的保证。因此,为了恢复退化草原生态系统功能,需要修复能导致微气候变化的植物群落结构,否则难以成功。 本研究立足于原创性的实验研究,在中国特有的自然草原生态系统上开展,结合不同温度梯度的三地区涡度相关系统进行了能量平衡闭合的移动比较实验,以及结合常用土地利用方式的定点能量平衡实验。在翔实的数据基础上,为涡度相关方法的陆地表面能量平衡失衡问题提供了解释。增加了对两个主要能量流——土壤热通量和净辐射空间变异规律的认识,研究对于能量平衡和湍流通量相关研究是有价值的。在三个代表性地区首次利用多个净辐射仪和土壤热通量板的结果与三个标准的涡度相关系统进行了比较,这类量化失衡原因的相关研究应受到高度重视并进一步拓展,以提高对能量失衡的认识,进而推进水热和碳循环研究向更深层次发展。