91 resultados para LI-7(N,GAMMA)LI-8


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A new measurement of proton resonance scattering on Be-7 was performed tip to the center-of-mass energy of 6.7 MeV using the low-energy RI beam facility CRIB (CNS Radioactive Ion Beam separator) at the Center for Nuclear Study of the University of Tokyo. The excitation function of Be-7 + p elastic scattering above 3.5 MeV was measured Successfully for the first time, providing important information about the resonance structure of the B-8 nucleus. The resonances are related to the reaction rate of Be-7(p.gamma)B-8. which is the key reaction in solar B-8 neutrino production. Evidence for the presence of two negative parity states is presented. One of them is a 2(-) state observed as a broad s-wave resonance, the existence of which had been questionable. Its possible effects on the determination of the astrophysical S-factor of Be-7(p.gamma)B-8 at solar energy are discussed. The other state had not been observed in previous measurements, and its spin and parity were determined as 1(-). (C) 2009 Elsevier B.V. All rights reserved.

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The band structures of wurtzite ZnO are calculated using the empirical pseudopotential method (EPM). The 8 parameters of the Zn and O atom pesudopotential form factors with Schluter's formula are obtained. The effective mass parameters are extracted by using k.p Hamiltonian to fit the EPM results. The calculated band edge energies (E-g, E-A, E-B, and E-C) at Gamma point are in good agreement with experimental results. The ordering of ZnO at the top of valence band is found to be A(Gamma(7))-B(Gamma(9))-C(Gamma(7)) due to a negative spin-orbit (SO) splitting. Based on the band parameters obtained, the valence hole subbands of wurzite ZnO/MgxZn1-xO tensile-strained quantum wells (QWs) with different well widths and Mg compositions are calculated using 6-band k.p method. (c) 2005 Elsevier B.V. All rights reserved.

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The band structures of wurtzite ZnO are calculated using the empirical pseudopotential method (EPM). The 8 parameters of the Zn and O atom pesudopotential form factors with Schluter's formula are obtained. The effective mass parameters are extracted by using k.p Hamiltonian to fit the EPM results. The calculated band edge energies (E-g, E-A, E-B, and E-C) at Gamma point are in good agreement with experimental results. The ordering of ZnO at the top of valence band is found to be A(Gamma(7))-B(Gamma(9))-C(Gamma(7)) due to a negative spin-orbit (SO) splitting. Based on the band parameters obtained, the valence hole subbands of wurzite ZnO/MgxZn1-xO tensile-strained quantum wells (QWs) with different well widths and Mg compositions are calculated using 6-band k.p method. (c) 2005 Elsevier B.V. All rights reserved.

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Three novel supramolecular assemblies constructed from polyoxometalate and crown ether building blocks, [(DB18C6)Na(H2O)(1.5)](2)Mo6O19.CH3CN, 1, and [{Na(DB18C6)(H2O)(2)}(3)(H2O)(2)]XMo12O40.6DMF.CH3CN (X = P, 2, and As, 3; DB18C6 = dibenzo-18-crown-6; DMF = N,N-dimethylfomamide), have been synthesized and characterized by elemental analyses, IR, UV-vis, EPR, TG, and single crystal X-ray diffraction. Compound 1 crystallizes in the tetragonal space group P4/mbm with a = 16.9701(6) Angstrom, c = 14.2676(4) Angstrom, and Z = 2. Compound 2 crystallizes in the hexagonal space group P6(3)/m with a = 15,7435(17) Angstrom, c = 30.042(7) Angstrom, gamma = 120degrees, and Z = 2. Compound 3 crystallizes in the hexagonal space group P6(3)/m with a = 15.6882(5) Angstrom, c = 29.9778(18) Angstrom, gamma = 120degrees, and Z = 2. Compound 1 exhibits an unusual three-dimensional network with one-dimensional sandglasslike channels based on the extensive weak forces between the oxygen atoms on the [Mo6O19](2-) polyoxoanions and the CH2 groups of crown ether molecules, Compounds 2 and 3 are isostructural, and both contain a novel semiopen cagelike trimeric cation [{Na(DB18C6)(H2O)(2)}(3)(H2O)(2)](3+). In their packing arrangement, an interesting 2-D "honeycomblike" "host" network is formed, in which the [XMo12O40](3-) (X = As and P) polyoxoanion "guests" resided.

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牡丹复合体属芍药属(Paconia)牡丹组(Sect. Moutan).原有6个种名,包括花壬 牡丹、名贵野生花卉紫斑牡丹,著名中药牡丹皮原植物,野生种类为我国特有,仅分 布在以秦岭为中心的较小区域.本研究从山西、陕西、河南、湖北、甘肃共采集14 个居群(包括复合体不同类型).通过野外居群调查、样方研究,移栽实验,以及细 胞学观察、孢粉学观察分析、种子蛋白和DNA水平多样性的探索性的工作,并结合 聚类分析方法,对牡丹复合体进行了分类学和保护生物学两方面的研究,主要结论 为: 1.本复合体为多年生木本植物,生长缓慢,在天然状况下,从种子播种到开花结实长达7年.枝条通常具隔年开花习性.严格单花顶生,花期短(5-10天).雄蕊先熟,以异花传粉为主(主要传粉者有甲虫和野蜂).自交亲和,甲虫在传粉过程中常常破坏心皮和胚珠.胚珠败育比例很高,紫斑牡丹50%.其它类群达90%. 2.种子生物学特性研究,发现本复合体种子属正统种子,但种子衰变快.种子萌发时间长,一般的化学及物理处理对种子萌发无明显促进作用,种子具上胚轴休眠特性.打破休眠需要两个条件:一是胚根长足3 cm.二是10℃左右的低温或GA3处理,野生紫斑牡丹种子较大,复合体其它野生类群种子较小.野生牡丹的种子活力相当低,萌发时间更长. 3.样方的调查统计表明,稷山和永济两地区的矮牡丹株数一龄级分布规律是2—5年生个体最多,随年龄级的增加,个体数目减少.居群呈增长趋势.紫斑牡丹株数一龄级分布规律是青壮年时期个体数目多,幼年时间和老年时期个体数目少,居群呈衰退的趋势,这与其本身繁殖方式和人为破坏程度相关. 4.对13个居群花粉扫描电镜观察表明,本复合体紫斑牡丹(P. rockii)为粗网纹,网眼大,其它类群为细网纹、网眼小. 5.通过18个居群的核型分析并结合前人工作,发现本复合体染色体数目稳定2n =10.核型差别不大,野生类群和栽培品种间有一定分化,但总体上核型多样性比较贫乏.通过8个居群C带研究,发现带纹很少,但多样性很丰富.8个居群表现出7种带型. 6.种子蛋白和DNA水平多样性的初步研究,发现复合体具有较丰富的多样性.但多样性的分布对类群的划分帮助不大,有待进一步研究. 7.通过形态性状分析发现产自各地区矮牡丹、河南粉花类型、神农架红花类型具根出条现象,并以此为主要繁殖方式,紫斑牡丹无此现象.神农架红花类型植株矮小,复合体其它类群较高.产自各地区的矮牡丹和神农架红花类型为二回三出复叶.小叶数目多为9.矮牡丹顶生小叶具浅裂、中裂或深裂,裂片具齿,神农架红花类型顶生小叶仅具浅裂或齿(全缘).河南粉花类型为二回羽状复叶.小叶数目12-15.紫斑类型叶为二回或三回羽状复叶、小叶数目15-40.小叶分裂方式分两种类型,秦岭西部居群以浅裂、全缘为主,东部居群以中裂或深裂为主,裂片具齿.神农架红花类型花为平展型、较小,其它地区花杯状、较大.花盘有二种类型.紫斑类群花盘黄色或白色.1/2-4/5包被心皮,心皮被稀疏长柔毛,其它类群花盘紫红色,全包心皮,心皮密被短硬毛.根据形态性状分析.并结合细胞学、孢粉学和地理分布研究,对复合体做如下处理:(l)把神农架红花类型做为新种处理P.quii Y.L.Pei et Hong.(2)保留P.rockii(S.G.Haw et L.A. Lanener)T.Hong ct J.J.Li和P.ostii T.Hong et J.X. Zhang.前者进一步分成二亚种:subsp. rockii和subsp. lanceolata Y.L.Pei et Hong(新亚种).后者包括河南粉花类型,中药丹皮原植物.(3)保留P.suffruticosa Andr.种内分二亚种:subsp. suffruticosa和subsp. spontanea (Rehd.)S.G. Haw et L.A, Lauener. (4)废弃P.papaveracea Andr.和P.jishanensis T.Hong et W.Z.Zhao (5)P.yanancnsis T.Hong et M.R.Li作为存疑种处理. 8.通过上述研究对野生牡丹濒危原因加以分析,认为致濒原因主要是人为干扰和种子萌发和传粉特点等生物学特性造成,但以前者为主,建议应广泛开展各个层次多样性研究,为生物多样性保护利用奠定基础。

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In the present paper, sorption, persistence, and leaching behavior of three microcystin variants in Chinese agriculture soils were examined. Based on this study, the values of capacity factor and slope for three MCs variants in three soils ranged from 0.69 to 6.00, and 1.01 to 1.54, respectively. The adsorption of MCs in the soils decreased in the following order: RR > Dha(7) LR > LR. Furthermore, for each MC variant in the three soils, the adsorption rate in the soils decreased in the following order: soil A > soil C > soil B. The calculated half-time ranged between 7.9 and 17.8 days for MC-RR, 6.0-17.1 days for MC-LR, and 7.1-10.2 days for MC-Dha(7) LR. Results from leaching experiments demonstrated that recoveries of toxins in leachates ranged from 0-16.7% for RR, 73.2-88.9% for LR, and 8.9-73.1% for Dha 7 LR. The GUS value ranged from 1.48 to 2.06 for RR, 1.82-2.88 for LR, and 1.76-2.09 for Dha(7) LR. Results demonstrated the use of cyanobacterial collections as plant fertilizer is likely to be unsafe in soils. (c) 2006 Elsevier Ltd. All rights reserved.

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Aspects of the biology of pond-cultured Chinese mitten crab (Eriocheir sinensis H. Milne-Edwards) were studied from June to November 1993. The survival rate of the population was estimated at 18.6%, and there was no significant difference between sexes in growth (t-test, P > 0.05). As the crabs grew from 7.3 to 33.8 mm in mean carapace length, seven molts were observed for the population. The intermolt period ranged from seven to 22 days and lengthened with increased size. Sex ratio at each sampling time did not differ significantly from 1:1 (Chi-square test, P > 0.05). Female crabs presumably required about eleven postlarval molts to reach sexually mature size, which was 34.1 +/- 3.9 (SD) mm. in carapace length in this study.

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Six-period 4 nm GaN/10 nm AlxGa1-xN superlattices with different Al mole fractions x were prepared on (0001) sapphire substrates by low-temperature metal-organic chemical vapor deposition. The linear electro-optic (Pockels) effect was studied by a polarization-maintaining fiber-optical Mach-Zehnder interferometer system with an incident light wavelength of 1.55 mu m. The measured electro-optic coefficients, gamma(13)=5.60 +/- 0.18 pm/V, gamma(33)=19.24 +/- 1.21 pm/V (for sample 1, x=0.3), and gamma(13)=3.09 +/- 0.48 pm/V, gamma(33)=8.94 +/- 0.36 pm/V (for sample 2, x=0.1), respectively, are about ten times larger than those of GaN bulk material. The enhancement effect in GaN/AlxGa1-xN superlattice can be attributed to the large built-in field at the interfaces, depending on the mole fraction of Al. (C) 2007 American Institute of Physics.

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The production of C, N, O elements in a standard big bang nucleosynthesis scenario is investigated. Using the up-to-date data of nuclear reactions in BBN, in particular the Li-8 (n, gamma) Li-9 which has been measured in China Institute of Atomic Energy, a full nucleosynthesis network calculation of BBN is carried out. Our calculation results show that the abundance of C-12 is increased for an order of magnitude after addition of the reaction chain Li-8(n, gamma) Li-9(alpha, n) B-12(beta) C-12, which was neglected in previous studies. We find that this sequence provides the main channel to convert the light elements into C, N, O in standard BBN.

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利用LI-6400CO2分析系统测定了长白山红松针阔叶混交林生态系统土壤呼吸、乔木和灌木树干和枝条的呼吸、植物叶片光合与呼吸.同步监测森林小气候气象因子,建立土壤、树干、叶片与气象因子间的模型.根据红松针阔叶混交林植被群落特性,估算红松针阔叶混交林森林生态系统不同组分CO2通量.利用涡度相关技术监测红松针阔叶混交林净生态系统交换量.探讨温度、光合有效辐射对森林生态系统CO2通量的影响.通过分析发现,在当年的气候条件下,该森林净生态系统交换量主要受土壤呼吸和叶片光合的影响.红松针阔叶混交林净生态系统交换量全年变化范围在-4.67~13.80μmol·m-2·s-1.该森林生态系统CO2通量在冬季和夏季里平均分别为-2.0和3.9μmol·m-2·s-1(24 h平均值).乔木、灌木和草本的初级生产力分别占阔叶红松林总初级生产力的89.7%,3.5%,6.8%.土壤呼吸是森林生态系统中最主要的CO2排放源,约占红松针阔叶混交林生态系统CO2排放的69.7%,植物叶片和枝干分别占15.2%和15.1%.在生长季和非生长季中红松针阔叶混交林净生态系统交换量分别占全年CO2通量的56.8%和43.2%.自养呼吸占总初级生产力的比值(Ra:GPP)为0.52(NPP:GPP=0.48).森林生态系统地下当年碳积累量占总初级生产力的52%.土壤呼吸占总初级生产力的60%.红松针阔叶混交林NPP为769.3 gC·m-2·a-1.该森林净生态系统交换量(NEE)为229.51 gC·m-2·a-1.涡度相关技术获得的该森林生态系统NEE低于箱式法获得的19.8%.

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A new acetylated flavanol, 3,7-O-diacetyl (-)-epicatechin (3), and seven known flavanol derivatives, (-)-epicatechin (1), 3-O-acetyl (-)-epicatechin (2), 3,3 ',4 ',5,7-O-pentaacetyl (-)-epicatechin (4), (+)-afzelechin (5), (+)-catechin (6), cinchonain Ib (7), and proanthocyanidin B2 (8), were isolated from the stems and twigs of the mangrove plant Rhizophora stylosa and identified. The crude extract, the different fractions and all of the purified compounds were evaluated for DPPH radical scavenging activity.

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One new sesquiterpene, (4E)-1-bromo-5-[(1'S*, 3'R*)-3'-bromo-2',2'-dimethyl-6'-methylenecyclohexyl]-3-methylpent-4-ene-2,3-diol (1), and fifteen known sesquiterpenes, isopalisol (2), luzonensol (3), palisadin B (4), aplysistatin (5), palisadin A (6), 4-hydroxyl-palisudin C (7), 5-acetoxypalisadin B (8), 10-hydroxyaristolan-9-one (9), aristol-8-en-1-one (10), aristolan-9-en-1-one (11), aristolan-1(10)-en-9-one (12), aristolan-1( 10)-en-9-ol (13), aristolan-1(10), 8-diene (14), aristolan-1,9-diene (15) and aristofone (16), were isolated from a sample of marine red alga Laurencia similis. Their structures were established by detailed NMR spectroscopic analysis and comparison with literature data. Compounds 2-9, and 16 were isolated for the first time from this species. All these metabolites were submitted for a cytotoxicity assay against the tumor cell line BEL7402 (human liver adenocarcinoma), but all of them were found inactive (IC50 > 10 mu g/mL).

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The aim of this study was to optimize the cryopreservation protocols for the sperm of red seabream, Pagrus major. The 2-mL cryovials and programmable freezer were employed for cryopreservation. Six extenders, six cryoprotectants in various concentrations ranging from 6 to 20% (v/v), four cooling rates, and three thawing temperatures were evaluated by postthaw sperm motility and fertility. The ratio of sperm to egg for postthaw sperm fertilization trials was experimentally standardized and was optimal at 500:1. The best motility of postthaw sperm (79.4 +/- 4.7% to 88.6 +/- 8.0%), fertilization rates (89.6 +/- 2.9 to 95.6 +/- 1.9%), and hatching rates (85.3 +/- 5.1% to 91.4 +/- 4.3%) were achieved when Cortland extender, dimethyl sulfoxide (15, 18, and 20%) or ethylene glycol (9, 12%) as cryoprotectants, 20 C/min as the cooling rate, and 40 C as the thawing temperature were employed. Moreover, the results on embryonic development were not significantly different between cryopreserved sperm and fresh sperm during incubation process. In conclusion, these methods of cryopreservation of red seabream sperm are suitable for routine aquaculture application and preservation of genetic resources.

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A new lead(II) phosphonate, Pb[(PO3)(2)C(OH)CH3]center dot H2O (1) was hydrothermally synthesized and characterized by IR, elemental analysis, UV, TGA, SEM, and single crystal X-ray diffraction analysis. X-ray crystallographic study showed that complex 1 has a two-dimensional double layered hybrid structure containing interconnected 4- and 12-membered rings and shows an unusual (5,5)-connected (4(7) . 6(3)) (4(8) .6(2)) topology. (C) 2008 Elsevier B.V. All rights reserved.

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理性力学基础》为《中国科学院研究生教学丛书》之一。
    《理性力学基础》系统地介绍了理性力学的主要科学体系和基本理论。《理性力学基础》由四部分,共十五章组成。第一部分综合介绍了理性力学的科学意义、方法和特点,从理性力学角度概括论述变形几何学与运动学、力学基本定律与场方程以及本构方程的一般原理。着重阐明张量和场方程的时空无差异原理,以及本构方程所应遵循的客观性原理。第二部分着重介绍简单物质的理论体系。作为典型范例进一步阐明弹性物质和简单流体的本构方程以及弹性体有限变形边值问题的分析方法。第三部分详细介绍黏弹性物质、弹塑性物质及晶体塑性的基本理论。第四部分主要介绍含缺陷物质的本构理论。
    《理性力学基础》可作为力学、应用数学、理论物理等专业的研究生教材,也可供力学工作者及高等院校力学专业教师参考。

目录 

第一章 绪论
1·1 理性力学目的和意义
1·2 理性力学的特点与体系
1·3 理性力学的方法
1·4 符号
第二章 变形几何学和运动学
2·1 直角坐标系的张量
2·2 物体的构形与运动
2·3 变形梯度
2·4 应变度量和面元、体元变形
2·5 应变率
第三章 基本定律与场方程
3·1 质量守恒定律
3·2 应力原理与动量守恒定律
3·3 能量守恒定律和熵定律
3·4 功共轭与应力度量
3·5 场方程
3·6 随体坐标系
第四章 本构方程的一般原理
4·1 时空系的变换
4·2 基本定律的客观性
4·3 本构方程的一般原理
第五章 简单物质
5·1 张量函数
5·2 张量函数表示定理
5·3 简单物质的本构方程
5·4 本构方程的简化形式
5·5 各向同性物质
5·6 简单固体
5·7 简单流体和流晶
5·8 内部约束
5·9 特殊类型物质
5·10 衰退记忆
第六章 弹性物质
6·1 弹性物质的本构方程
6·2 物质对称性
6·3 各向同性弹性固体
6·4 超弹性物质
6·5 各向同性超弹性物质
6·6 主轴表示
6·7 储能函数表示式
6·8 二次弹性
6·9 均匀变形场
6·10 储能函数的实验确定
第七章 弹性体有限变形边值问题
7·1 边值问题的提法
7·2 若干典型问题
7·3 平面应变问题
7·4 不可压缩各向同性弹性体
第八章 简单流体
8·1 直线流动
8·2 曲线流动
8·3 伸长历史恒定运动
8·4 定常测黏流动
8·5 Poiseuille流动
8·6 Couette流动
8·7 圆锥-平板流动
8·8 端部正应力效应
8·9 Stokes流体测黏流动
8·10 定常拉伸流动
第九章 黏弹性物质
9·1 线性黏弹性理论
9·2 非线性黏弹性固体
9·3 本构泛函展开
9·4 非线性黏弹性流体
第十章 弹塑性物质
10·1 微小变形塑性理论
10·2 张量的时间导数
10·3 有限塑性变形的本构方程
10·4 塑性大变形基本方程
10·5 Drucker公设与有限塑性变形
第十一章 晶体塑性理论
11·1 晶体塑性变形运动学
11·2 硬化规律
11·3 硬化系数表示式
11·4 晶体塑性本构关系
11·5 滑移剪切率γ(α)的存在性与惟一性
11·6 率相关流动规律
第十二章 缺陷连续统的线性理论
12·1 张量场的微分运算
12·2 协调条件
12·3 缺陷的几何意义
12·4 位错弹性理论
12·5 位错塑性理论
12·6 一般缺陷塑性理论
12·7 晶体塑性位错理论
12·8 Nye张量及缺陷塑性理论小结
12·9 位错塑性理论二维公式及算例
第十三章 非黎曼几何及流形简介
13·1 Euler空间张量场的绝对微分
13·2 曲率张量
13·3 线性空间
13·4 仿射联络空间
13·5 非完整变换
13·6 拓扑空间
13·7 微分流形
第十四章 缺陷连续统的非线性理论
14·1 非Niemann物质流形的构造
14·2 缺陷的几何意义
14·3 缺陷连续统的弹性理论
14·4 缺陷连续统的塑性理论
14·5 晶体塑性位错理论
第十五章 理性力学若干应用
15·1 有限变形的精确描述
15·2 曲线坐标的相应公式
15·3 本构方程的客观性原理
15·4 物质对称性
15·5 主轴法
15·6 客观应力率
附录 曲线坐标
1 基向量与度量张量
2 逆变导数
3 应力张
4 运动方程