从铁磁到振荡状态的不连续相位过渡在一个不平衡的平均场旋转模型中
1Université Grenoble Alpes, CNRS, LIPhy, 38000 Grenoble, France.
Physical review. E
|April 18, 2024
概括
我们通过引入非互惠合,在旋转模型中发现了一个新的振荡磁相. 这个阶段表现出独特的过渡和稳定性质,影响了我们对不平衡磁力的理解.
科学领域:
- 统计物理学的统计物理.
- 凝聚物质物理学 凝聚物质物理学
- 磁力学 磁力学 是一种
背景情况:
- 铁磁模型通常表现出偏磁或铁磁相.
- 没有平衡的系统可以显示出在平衡状态下看不到的复杂的新兴行为.
研究的目的:
- 为了研究一个不平衡的铁磁平均场旋转模型.
- 描述一个具有磁化自发时间振荡的新阶段.
主要方法:
- 引入具有非互惠合的动态场变量.
- 确定一个不平衡的兰道自由能量概括.
- 使用大偏差函数和平滑的随机时间衍生品进行分析.
主要成果:
- 确定一个偏磁,铁磁和振荡相.
- 连续的 (偏磁振荡) 和不连续的 (铁磁振荡) 过渡的特征.
- 观察相位共存 (稳定/超稳定) 和对参数值的依赖.
结论:
- 这项研究揭示了不平衡磁力学中一个新的振荡阶段.
- 不平衡的动态导致复杂的阶段过渡和稳定性景观.
- 的产生在共存区域显示为最大,取决于系统的大小.
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