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The starting cluster of a run is coded as an offset to the starting cluster of the previous run. Length and starting cluster are variable size fields.

起始号和长度存储于变长的域中,一个RUN的第一个字节表明了起始号和的个数分别占用的字节数,跟着的个数数据,接着是起始号的数据。

Our results reveal that with the same number of cobalt atoms and the same cobalt-substrate interation stength, the melting points and pre-melting intervals of the two kinds of supported Co clusters are all in reasonable agreement with each other. With increasing the depth of supported potential, the melting points increase for the supported cluster. Similar to the case of free clusters, the linear relation between the melting point and the inverse of cluster's size cube root is also found for the two kinds of supported clusters.

结果表明:对于给定原子数目的支撑Co团,在衬底势强度相同时,两种衬底势下对支撑团熔点及预熔化区间给出了一致的描述;随衬底势强度增加,支撑团熔点升高,且两种衬底势所描述的支撑Co团也类同于自由Co团都表现出较好的熔点与尺寸依赖的线性关系。

In homogeny cluster head hierarchical topology, the article first discusses the selection of cluster head. With a given formula on weights, a suitable cluster head node is selected. And according to the relationship of location with cluster head node, the gateway nodes and the distributed gateway nodes are selected.

头同构的分算法中,首先讨论了头的选择,给出了一个权值设定公式,按照权值大小,选择出合适的头节点,然后根据和头节点的位置关系,确定网关节点和分布式网关节点。

The structures and stabilities of the ground-states for Cu13-nAgn clusters have been studied by Gupta model potential based on tight binding second moment approximation in combination with a genetic algorithm. It is found that the lowest energy structures of the pure clusters (n=0,13) are perfect icosahedron, and the structures for the bimetallic clusters (n=1~10) have stable structure which are slightly deformed with respect to the perfect icosahedron, The Cu atom prefers to occupy the center of the clusters with higher coordination numbers.

在混合团基态结构优化的遗传算法方案中增加了交换算子,结合Gupta紧束缚模型势研究了Cu13-nAgn团的最低能量结构,选择合适的交换和杂交概率,可有效地提高优化效率,优化结果表明,Cu13和Ag13是全对称的二十面体,n=1~10的混合团能形成稳定结构,其构型是在二十面体基础上发生畸变,Cu原子趋于处在团中心,随着Ag原子数目的增加,原子间的平均距离单调增加,团的结合能单调减小,Cu2Ag12和CuAg12只存在亚稳结构。

The results show that the sturcture of each of Tin clusters is obtained by capping one Ti atom to the Tin-1. The Natural bond orbital analysis show that the 4s , 4p, 4d orbitals hybridizes with 3d orbital, and about one electron transfer from 4s orbital to 3d orbital. Moreover, the electrons also transfer between different atom. The results also indicate that the average bond length of clusters were determined by the 4d and 3d orbitals except Ti7. But for Ti7, the average bond length only depend on 3d orbital.

研究结果表明: Tin(n=2~7)团都依带帽的形式在前一个团的结构基础上加一个原子变化而来;通过自然轨道分析发现,团原子的轨道存在sp-d杂化,有大约一个电子从4s转移到了3d,原子之间亦存在电子转移,而且除Ti7外,团键长由最外层4d轨道电子和3d轨道共同决定,在Ti7中,团键长由3d轨道决定。

The results show that the radiative properties of randomly distributed soot aggregates for a given fractal dimension are complex functions of the monomer diameters, the number of monomers in the aggregates,and the refractive index; For a small value of the monomer diameters, the absorption cross section of soot aggregates tends to be relatively constant when the fractal dimension is small but increases rapidly when the fractal dimension exceeds two. However, a monotonical reduction in light absorption with the increase of the fractal dimension is observed for soot aggregates with sufficiently large monomer diameters, number of monomers,and refractive index. The scattering cross section , extinction cross section and single-scattering albedo increase monotonically with the increase of the fractal dimension. Overall, the results for soot aggregates differ profoundly from those calculated for the equivalent spherical particles, and the discrepancies between them will change small with the increase of the fractal dimension.

研究表明,在给定分形维数的情况下,烟尘団粒子的辐射特性取决于原始微粒粒径、数量及复折射率;原始微粒较小的団粒子,当分形维数较小时,吸收截面变化不明显,但当分形维数大于二时,吸收截面骤然增大,然而,对于具有比较大的原始微粒粒径、数量及复折射率的烟尘団粒子,吸收截面随着分形维数的增大而单调递减;随着分形维数的增大,団粒子的散射截面、消光截面及单次散射反照率均单调递增;从整体上来讲,団粒子的辐射特性与等效球形粒子的辐射特性存在着比较大的差别,并且这种差别随着分形维数的增大而减小。

A distributed secure clustering protocol is proposed, in which the secure network initialization, random number broadcast from the base station and one-way hash chain are used to achieve the resiliency against possible attacks including node personating, cluster-head occupying, malicious cluster-member recruiting and multiple cluster-membership attacks.

针对成协议所面临的各种安全威胁,提出了一种分布式安全成协议,通过网络安全初始化、可信基站的随机数广播和单向密钥链技术来有效地抵御节点伪装和首占据攻击、成员恶意征募攻击和多重成员身份攻击。

We led the density function into the data structure as the weight, and use dense micro-cluster to describe the arbitrary-shaped clusters in data streams. In addition, we propose candidate core-micro-cluster and isolated micro-cluster synopses to maintain and distinguish the potential micro clusters and isolation point in data streams.

我们把密度函数以权值的形式引入数据结构中,并利用核心微描述数据流中任意形状的,并提出候选核心微和孤立微结构分别用于维护并区分数据流中潜在的核心和孤立点。

The calculated results show that azido in azides has linear structure , the most optimized CaN6 has linear structure , and the most optimized (CaN6)n (n=2~5) clusters have chain structure of perpendicularity of approximate diamond composed by two azido with two Ca atoms . The middle N atoms of azido show positive, the N atoms at both ends of azido show negative, and the N atoms effected with Ca atoms directly show more negative . There is strong ionic bond between the Ca and N atoms. The IR spectra of the most optimized (CaN6)n (n=1~5) clusters have four vibrational sections , the whole strongest vibrational peak lies in 2195~2280cm-1,and the vibrational mode is anti-symmetric stretching vibration of N-N bonds in azido . Stability analysis show that (CaN6)3 and (CaN6)5 clusters are more stable than other clusters .

结果表明,叠氮化合物中叠氮基以直线型存在,CaN6团的最稳定结构为线型结构,(CaN6)n(n=2~5)团首先由两个叠氮基与两个Ca原子构成一个近似菱形,再由菱形相互垂直形成链状最稳定结构;叠氮基中间的N原子显示正电性,两端的N原子显示负电性,且与Ca直接作用的N原子负电性更强,金属Ca原子和N原子之间形成很强的离子键;(CaN6)n(n=1~5)团最稳定结构的IR光谱分为4个部分,其最强振动峰均位于2195~2280cm-1,振动模式为叠氮基中N-N键的反对称伸缩振动;稳定性分析显示,(CaN6)3和(CaN6)5团相对于其他团较为稳定。

The numbers of clusters made up of 1551 and 1541 bonded pairs representing the non-crystal structure occupy predominate position and the small numbers of clusters made up of 1431, 1661 and 1441 bonded pairs coexist in the non-crystal system at 4×10〓K/s cooling rate, thus there exist a large number of icosahedra clusters in the non-crystal system. The numbers of clusters made up of 1421 bonded pairs corresponding to the fcc-like structure occupy predominate position and the small numbers of clusters made up of 1422 and 1551 bonded pairs coexist in the crystal system during the 4×10〓K/s cooling process, thus the system can form the regular fcc-like structure.

在4×10〓K/s的冷速下,标征体系非晶结构的五重对称键型1551和1541所形成的小团数量在非晶体系中占主导位置,同时还存在少量的1431、1441和1661等其它键型形成的小团,这样,体系中含有大量的二十面体团结构;在4×10〓K/s的冷速下,标征面心立方结构的1421键型所形成的小团数量在晶体中占第一位,同时还存在一定量的1422、1441和1661等其它类型的键对所形成的团,体系最终形成面心立方结构。

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