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1)  move neighborhood
移动邻域
2)  neighborhood moving
邻域移动
1.
A tabu search with double neighborhood moving is proposed according to characteristics to solve knapsack problem.
基于背包问题的特征,提出了基于双邻域移动和双禁忌表的禁忌搜索算法:第一种邻域移动的物理意义是增加背包中的物品数量,第二种邻域移动的物理意义是交换背包内外的不同物品。
3)  moving average nearest neighborhood forecasting method
移动平均最近邻域法
1.
We present a new forecasting method-moving average nearest neighborhood forecasting method,which is based on the phase space reconstruction and combining with the moving average forecasting and the nearest neighbor.
提出了一种新的基于相空间重构和移动平均相结合的预测方法——移动平均最近邻域法,从理论与实际数据两方面分析和验证了该方法对短时交通流预测的有效性。
4)  Dynamic Neighborhood
动态邻域
1.
The Stream of vehicles Detection of Intersection Based on Dynamic Neighborhood;
基于动态邻域的交叉路口车流检测
2.
Research on particle swarm optimization based on dynamic neighborhood
基于动态邻域的粒子群算法的研究
3.
NNI_PSO incorporates near neighbor interaction into the PSO’s velocity updating equation,meanwhile,combines with "fittest exist" by which introduces dynamic neighborhood structure and inertia weight nonlinearly varying into the PSO.
NNI_PSO在PSO算法的速度更新公式中增加了近邻交互部分,并结合"优胜劣汰",引入动态邻域结构和惯性权值非线性变化。
5)  moving neighborhood
滑动邻域
1.
Method of determining moving neighborhood based on range
基于变程的滑动邻域确定方法
6)  8 neighborhood translation
8邻域平移式
1.
Four edge correction methods of the buffer zone,the 8 neighborhood reflection,the 8 neighborhood translation and the distance determinant method of the 4 th neighborhood on the neighborhood were compared with mingling index and angle index of tree spatial structure parameters and the ratio of the trees taken part in the calculation.
选择1块100m×100m的实地调查样地并设置10块100m×100m的模拟样地,从空间结构参数大小比数、混交度和角尺度以及参与计算的株数比例等方面对距离缓冲区、8邻域对称式、8邻域平移式和第4邻体距离判定法这4种边界校正方法进行比较。
补充资料:超导电性的局域和非局域理论(localizedandnon-localizedtheoriesofsuperconductivity)
超导电性的局域和非局域理论(localizedandnon-localizedtheoriesofsuperconductivity)

伦敦第二个方程(见“伦敦规范”)表明,在伦敦理论中实际上假定了js(r)是正比于同一位置r的矢势A(r),而与其他位置的A无牵连;换言之,局域的A(r)可确定该局域的js(r),反之亦然,即理论具有局域性,所以伦敦理论是一种超导电性的局域理论。若r周围r'位置的A(r')与j(r)有牵连而影响j(r)的改变,则A(r)就为非局域性质的。由于`\nabla\timesbb{A}=\mu_0bb{H}`,所以也可以说磁场强度H是非局域性的。为此,超导电性需由非局域性理论来描绘,称超导电性的非局域理论。皮帕德非局域理论就是典型的超导电性非局域唯象理论。

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