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moving glass phase
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  moving glass phase
This new fixed point describes the moving glass phase at T = 0.
      
For the dynamics the very question of the presence of topological defects in the moving glass phase is at stake.
      


We have investigated the vortex density effects on the vortex motion in type II superconductors. By calculating the vortex velocity, differential resistance, longitudinal voltage noise and static structure factor in two-dimensional disorder pinning vortex lattices, a dynamical phase diagram has been obtained with varying vortex density. With the driving force increased, the five phases appear one after another: the pinning glass phase, plastic flow phase, smectic flow phase, and moving glass phase, and...

We have investigated the vortex density effects on the vortex motion in type II superconductors. By calculating the vortex velocity, differential resistance, longitudinal voltage noise and static structure factor in two-dimensional disorder pinning vortex lattices, a dynamical phase diagram has been obtained with varying vortex density. With the driving force increased, the five phases appear one after another: the pinning glass phase, plastic flow phase, smectic flow phase, and moving glass phase, and the last one including the moving transverse glass and Bragg glass phases. A higher vortex density is favorable to the formation of the ordered vortex lattice. With increasing vortex density, the smectic flow regime disappears gradually. As the vortex density is increased beyond a critical value, the smectic flow phase disappears, exhibiting a transition from the plastic flow phase to the moving glass phase.

计算了二维无序钉扎系统中磁通运动的平均速度、微分电阻、纵向电压噪声和静态结构因子 .通过在不同磁通密度下的磁通运动形式 ,给出了磁通运动的动力学相图 .研究表明 ,磁通晶格存在钉扎相、塑性流相、近晶流相 ,和运动玻璃相 .在运动玻璃相中 ,随着驱动力的进一步增加 ,横向玻璃态和运动Bragg玻璃态相继出现 .磁通密度增大有利于有序相的出现 .当磁通密度增大到一定程度时 ,近晶流动相会消失 .磁通运动随着外加驱动电流增大发生从塑性流动相到运动玻璃相的转变

 
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