对不均的艾伦-卡恩平均曲率的能量量化
Huy The Nguyen1, Shengwen Wang1
1School of Mathematical Sciences, Queen Mary University of London, Mile End Road, London, E1 4NS UK.
概括
这项研究分析了艾伦-卡恩相位过渡,揭示了在相场极限中的迪里克莱特和潜在能量之间的等能量分布. 相关的变量汇聚到一个整数可纠正的变量,扩展艾拉德.
科学领域:
- 几何测量理论 几何测量理论
- 部分微分方程部分微分方程.
- 微分几何学的差异几何学
背景情况:
- 艾伦-卡恩方程模型的阶段过渡,涉及与表面能量的接口.
- 了解这些接口在消失接口宽度的极限中的行为至关重要.
- 之前的工作建立了相场模型和尖接口界限之间的联系.
研究的目的:
- 分析与阿伦-卡恩相位过渡相关的Riemannian多重体上的多重体.
- 为了研究相场极限中变形体的能量分布和收性质.
- 在相变的背景下,扩展现有对变折的收定理.
主要方法:
- 使用艾伦-卡恩平均曲率 (艾伦-卡恩能量的第一个变化) 上的积分边界.
- 应用几何测量理论的技术来研究变形.
- 分析系统在相场极限中的行为.
主要成果:
- 在相场极限中证明了迪里克莱特和潜在能量之间的能量均分布.
- 表明与总能量相关的变量汇聚到一个整数可纠正的变量.
- 确定这个限制变量体在L^2中具有平均曲率,这是阿拉德定理的扩散版本.
结论:
- 艾伦-卡恩相位过渡在极限中表现出平衡的能量分布.
- 多元的融合为理解分散接口提供了一个严格的数学框架.
- 这项工作提供了关于与接口现象相关的多重融合的概括视角.
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