具有拓扑距离的群的循环态和相干态

B. Bhattacherjee, K. Bhattacharya, S. S. Manna
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引用次数: 4

摘要

研究了一组移动智能体二维集体运动的简单模型。像鸟类一样,这些智能体在开放的自由空间中移动,其中每个智能体与前n个邻居相互作用,这些邻居由具有自由边界条件的拓扑距离决定。使用与带有标量噪声的Vicsek模型中使用的相同的相互作用处方,可以观察到,在没有噪声的情况下,群达到了许多有趣的平稳状态。在“单汇状态”下,整个群体保持着完美的凝聚力和连贯性。在“循环状态”中,每个agent执行一个均匀的圆周运动,而整个群体执行一个脉动动力学,即在群体的最小和最大尺寸之间周期性地膨胀和收缩。当交互区的刷新速度最快时,整个群被分割成不同大小的更小的簇。在引入标量噪声的情况下,当介质从弹道运动过渡到扩散运动时,观察到一个交叉。预期的交叉时间依赖于噪声$\eta$的强度,并随着$\eta$发散到0$。在简单的版本中,agent的平移自由度被抑制,但它们的角运动被保留。这里的代理是自旋,放置在具有周期性边界条件的方形晶格的位置上。每个自旋都与其n = 2,3或4个最近的邻居相互作用。在稳态中,当相互作用为各向异性且$n$ = 2和3时,整个自旋模式作为一个整体运动;但是当相互作用是各向同性的,n=4时,它就完全冻结了。这些自旋构型具有涡-反涡对,其密度随着噪声$\eta$的增加而增加,并遵循优秀的有限尺寸缩放分析。
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Cyclic and coherent states in flocks with topological distance
A simple model of the two dimensional collective motion of a group of mobile agents have been studied. Like birds, these agents travel in open free space where each of them interacts with the first $n$ neighbors determined by the topological distance with a free boundary condition. Using the same prescription for interactions used in the Vicsek model with scalar noise it has been observed that the flock, in absence of the noise, arrives at a number of interesting stationary states. In the `single sink state' the entire flock maintains perfect cohesion and coherence. In the `cyclic state' every agent executes a uniform circular motion, and the entire flock executes a pulsating dynamics i.e., expands and contracts periodically between a minimum and a maximum size of the flock. When refreshing rate of the interaction zone is the fastest, the entire flock gets fragmented into smaller clusters of different sizes. On introduction of scalar noise a crossover is observed when the agents cross over from a ballistic motion to a diffusive motion. Expectedly the crossover time is dependent on the strength of the noise $\eta$ and diverges as $\eta \to 0$. In simpler version the translational degrees of freedom of the agents are suppressed but their angular motion are retained. Here agents are the spins, placed at the sites of a square lattice with periodic boundary condition. Every spin interacts with its $n$ = 2, 3 or 4 nearest neighbors. In the stationary state the entire spin pattern moves as a whole when interactions are anisotropic with $n$ = 2 and 3; but it is completely frozen when the interaction is isotropic with $n=4$. These spin configurations have vortex-antivortex pairs whose density increases as the noise $\eta$ increases and follows an excellent finite-size scaling analysis.
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