218 resultados para RB Patología


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本文系统地研究了化合物ASm_2I_5(A=K,Rb,Cs,T1)固体粉末的荧光光谱和反射光谱.讨论了Sm~(2+)在立方晶体场中的分裂能随着碱金属离子半径的增大而减小和f-d激发能随着A-I(A=Rb,T1)键的共价性增加而明显降低的现象.并从晶场效应和化学键性质两个方面解释了ASm_2I_5(A=K,Rb,Cs)和ASm_2I_5(A=Rb,T1)中的Sm~(2+)荧光光谱分别发生蓝移和红移的现象.

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位于四川西北部的马脑壳金矿床为陕甘川金三角区内一重要矿床,许多学者对其进行过大量的研究,对其地质地球化学特征有了较为全面的认识,同时对矿床的成因也做了多方面的探讨。为了确定矿床的成矿时代,从层状矿体中采集了富含流体包裹体的石英矿物。通过测定包裹体的Rb-Sr同位素组成,应用ISOPLOT程序计算获得(210±35)Ma的成矿年龄,该年龄与容矿地层的形成时代相近。流体包裹体的锶同位素初始比值与三叠纪时期海水的锶同位素比值相一致。综合矿体产出特征、矿石组构及区域构造演化历史,认为作为矿床主体的层状矿体是同生沉积的产物,脉状网脉状矿体则是由后期造山运动体制下所产生的成矿热流体沿裂隙构造交代充填所形成。

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在滇黔相邻地区,二叠纪宣威组下部发育一层硅质页岩和碳质页岩。页岩层位稳定、分布广泛,与下伏 峨眉山玄武岩组上部凝灰岩层呈假整合接触关系。用迭代法恢复硅质页岩的Rb-Sr同位索古混合线,得到硅 质页岩的年龄为(255 4-12)Ma。这个年龄不仅支持地层古地磁研究结果,而且符合地层年代学研究结果,表明 Rb-Sr同位索古混合线年代学方法在中生代地层能够适用。这个年龄与普遍认为的峨眉山玄武岩主喷发期258 Ma从时代关系上相符,而且有效地约束了峨眉山玄武岩喷发的上限。

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The deformation of alkali metals K, Rb, and Cs under epitaxial deformation is studied via the ab initio pseudopotential plane wave method using the local-density approximation. Under loading from the stable fee phase, metastable stares along directions [001], [111], and [201] are identified. One metastable state, presented at direction [201], has a very low symmetry in contrast to the planes [001] and [201]. Our results show that the softening direction and sequences of growth is significantly affected by the existence of the metastable states and magnitude of the energy barrier. The resulting softening sequences from soft to hard are [201], [110], [001], and [111] under biaxial compression and [001], [111], [201], and [110] under biaxial tension. An orthorhombic deformation path is used to investigate the fact, that the structure of the alkali films K and Cs evolve from the quasihexagonal structure into the (110)-oriented bcc structure, observed by experiments.

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本文讨论了利用赝势理论,按照Born稳定性判据,计算简单金属理论强度的方法。然后计算了六种简单金属(Li,Na,K,Rb,Cs和Pb)在0K和[100]单轴应力下的理论拉伸与压缩强度。

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本文根据经典力学的稳定性条件,用膺势方法导出了立方晶体在流体静负载下的经典稳定性判据:B(P)>0,C′(P)>0和C(P)>0。然后计算了七种简单金属(Li,Na,K,Rb,Cs,Al和Pb)在零温和流体静负载下的稳定性范围与理论拉伸强度。

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本文利用单参数Heine-Abarenkov模型势及Hubbard-Sham介电函数计算了七种简单金属(Li,Na,K,Rb,Cs,Al和Pb)的二阶与三阶弹性常数,两个可调参数用零温零压下晶体的弹性常数C_(44)与晶格常数的实验值来确定,计算结果与实验值或其他作者的理论计算值符合得比较好,尤其是Al的三阶弹性常数,本文的计算结果比其他作者的计算结果更接近于实验值。

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本文基于第一原理的能量计算和稳定性理论,研究了双原子组分材料β-SiC在各种载荷方式下的力学性质:弹性行为、应力-应变关系、稳定性和强度。由于沿[111]方向加载时四个Si-C键是不等价的,所以有相对内位移出现。本文的分析揭示了如下事实:当载荷较小时,内位移的影响不明显;当载荷较大时,影响则越来越显著;裂纹在{111}shuffle面上成核,并最终导致材料以解理的形式破坏。在沿[001]单轴拉伸的情况下,spinodal失稳(即体破坏)和Born失稳被同时触发,并体现了一种级联破坏的模式。基于同样的理论和方法,进一步研究了铝在各种加载方式下的响应及分叉行为。得到了铝的沿[001]和[111]方向单轴加载和单轴应变、及沿[010]和[001]方向的双轴比例加载情况下的、完整的能量-应变曲线和应力-应变曲线。详细地分析了沿[001]方向的单轴加载情况下的稳定性及分叉行为。研究结果表明,除了自然的面心立方结构外,所有其它的、应力自由的立方结构都是不稳定的。对于铝而言,稳定的面心立方结构不能从沿任何等价的[001]和[111]方向的单轴压缩的方法而得到。本文的结果丰富了现存的第一原理数据库。基于第一原理的能量计算,分析了碱金属K、Rb和Cs在如下四个结晶面上外延成长的行为,即{001}、{110}、{111}和{201}。发现除了在{110}面以外,在其它的三个结晶面上都发现有亚稳态存在。当外延应变为拉伸状态时,在{001}和{111}面上存在着亚稳态,其结构为b.c.c.结构。当外延应变为压缩状态时,在{201}面存在一个亚稳态,是一个超结构,。亚稳态的存在显著地影响着材料外延成长的软化行为。基于正交变形路径,并考虑了温度的影响以后,解释了实验上观察到的碱金属从h.c.p.结构转变到b.c.c.结构的现象。本文第五章归纳整理在赝势平面波框架下的总能、力和应力在实空间和动量空间的解析表达式,以方便参阅和使用。

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We measure the signal amplitude and linewidth of a dark line in coherent population trapping in the Rb vapour cell filled with mixed buffer gas N-2 and Ar as a function of cell temperature. We find that the dark line signal amplitude increases with temperature up to a maximum at 49 degrees C and then drops at higher temperatures due to quenching effects of N-2. The linewidth of the dark line remains basically constant, at 1080 Hz. We also measure the linewidth of the dark line as a function of laser intensity. The linewidth increases linearly with laser intensity. An intrinsic linewidth (FWHM=896 Hz at 3.4 GHz) of the Rb cell is obtained.

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对自行研制的激光冷却铷原子喷泉钟的微波谐振腔进行了分析和设计,确定了需要的微波谐振腔基本参数。对影响微波谐振腔共振频率的因素进行了分析和研究,得到了共振频率随环境因素的变化规律。这些对调节微波腔共振频率和提高原子钟的准确度有重要意义。还对研制的微波谐振腔进行了测试,结果表明微波谐振腔的性能满足激光冷却铷原子喷泉钟的要求。由测试结果进一步估算了微波谐振腔引起的横向腔相移。

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We experimentally study the ac Stark splitting in D2 line of cold Rb-87 atoms. The frequency span between the Autler-Townes doublets is obviously larger than that derived from theoretical calculation. Two physical effects, which increase the effective Rabi frequency, contribute to the splitting broadening. First, atoms tend to distribute in strong lield places of a inhomogeneous red-detuned light field. Second, atoms reabsorb scattered light when they are huge in number and high in density.