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首页> 外文期刊>Physical Review, B. Condensed Matter >Nonequilibrium dynamic phases and plastic flow of driven vortex lattices in superconductors with periodic arrays of pinning sites
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Nonequilibrium dynamic phases and plastic flow of driven vortex lattices in superconductors with periodic arrays of pinning sites

机译:具有钉扎点周期阵列的超导体中非平衡动力学相和驱动涡旋格的塑性流动

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摘要

We present results from an extensive series of simulations and analytical work on driven vortex lattices interacting with periodic arrays of pinning sites. An extremely rich variety of dynamical plastic flow phases, very distinct from those observed in random arrays, are found as a function of an applied driving force. Signatures of the transitions between these different dynamical phases appear as very pronounced jumps and dips in striking voltage-current V(I) curves that exhibit hysteresis, reentrant behavior, and negative differential conductivity. By monitoring the moving vortex lattice, we show that these features coincide with pronounced changes in the microscopic structure and transport behavior of the driven lattice. For the case when the number of vortices is greater than the number of pinning sites, the plastic flow regimes include a one-dimensional (1D) interstitial flow of vortices between the rows of pinned vortices, a disordered flow regime where 2D pin-to-pin and winding interstitial motion of vortices occurs, and a 1D incommensurate flow regime where vortex motion is confined along the pinning rows. In the last case, flux-line channels with an incommensurate number of vortices contain mobile flux discommensurations or "flux solitons," and commensurate channels remain pinned. At high driving forces, the 1D incommensurate paths of moving vortices persist with the entire vortex lattice flowing. In this regime, the incommensurate channels move at a higher velocity than the commensurate ones, causing incommensurate and commensurate rows of moving vortices to slide past one another. Thus there is no recrystallization at large driving forces. Moreover, these phases cannot be described by elastic theories. Different system parameters produce other phases, including an ordered channel flow regime, where a small number of vortices are pinned and the rest of the lattice flows through the interstitial regions, and a vacancy flow regime, which occurs when the number of vortices is less than the number of pinning sites. We also find a striking reentrant disordered-motion regime in which the vortex lattice undergoes a series of order-disorder transitions that display unusual hysteresis properties. By varying a wide range of values for the microscopic pinning parameters, including pinning strength, radius, density, and the degree of ordering, as well as varying the commensurability of the vortex lattice with its pinning substrate, we obtain a series of interesting dynamic phase diagrams that outline the onset of the different dynamical phases. We show that many of these phases and the phase boundaries;can be well understood in terms of analytical arguments. [References: 81]
机译:我们提出了一系列与驱动钉扎点的周期性阵列相互作用的驱动涡旋晶格的模拟和分析工作的结果。发现动态塑料流动相的种类非常丰富,与随机阵列中观察到的非常不同,它们是所施加驱动力的函数。这些不同的动态相位之间的跃迁的特征表现为在显着的电压-电流V(I)曲线中表现出明显的跳跃和下降,这些电压-电流V(I)曲线显示出磁滞,折返行为和负微分电导率。通过监视移动的涡流晶格,我们表明这些特征与从动晶格的微观结构和传输行为的明显变化相吻合。对于旋涡数大于固定点数的情况,塑性流动模式包括一排固定的旋涡之间的一维(1D)间隙气旋流动,其中2D销钉至销钉的无序流动状态发生涡旋的销和绕组间隙运动,并且一维不相称的流动状态,其中涡流沿钉扎行受限。在最后一种情况下,涡流数量不等的通量线通道包含流动通量不平衡或“磁通孤子”,而相应的通道则保持固定状态。在高驱动力下,运动涡旋的一维不相称路径随着整个涡旋晶格流动而持续存在。在这种情况下,不相称的通道以比相称通道更高的速度运动,导致不相称和相称的运动涡流相互滑过。因此,在大的驱动力下没有重结晶。而且,这些阶段不能用弹性理论来描述。不同的系统参数会产生其他阶段,包括有序通道流态,其中固定了少量的涡流,其余晶格流过间隙区域;以及空位流态,当涡流数量小于固定站点的数量。我们还发现了一种引人注目的折返无序运动机制,其中涡旋晶格经历了一系列显示异常磁滞特性的有序无序过渡。通过改变微观钉扎参数的宽范围值,包括钉扎强度,半径,密度和有序度,以及改变涡旋晶格与其钉扎衬底的可比性,我们获得了一系列有趣的动态相位概述了不同动力学阶段的开始的图表。我们表明,许多相位和相位边界都可以根据分析论点很好地理解。 [参考:81]

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