多温度原子组合:在超快电子激发后的无平衡演变.
Nikita Medvedev1,2, Alexander E Volkov3
1Institute of Physics of the <a href="https://ror.org/02yhj4v17">Czech Academy of Sciences</a>, Na Slovance 1999/2, 182 21 Prague 8, Czech Republic.
Physical review. E
|September 19, 2024
概括
超快激光照射在固体中产生一个多温度状态,在动量和配置子空间中具有单独的原子平衡. 这种非平衡状态最终会平衡,为新的热传输模型提供信息.
科学领域:
- 凝聚物质物理学 凝聚物质物理学
- 材料科学 是一种材料科学.
- 物理化学 物理化学
背景情况:
- 超快激光辐射和粒子束激发固体中的电子系统,导致暂时的热不平衡.
- 在这个过程中,电子和原子子系统都可以远离平衡.
研究的目的:
- 从第一原则来定义电子激发固体中的原子温度.
- 通过电子刺激诱导的非热相过渡期间研究原子温度的行为.
- 为多温度热传输方程提出一个公式.
主要方法:
- 对激发组合的原子温度定义的导出.
- 在动量子空间中分析运动温度.
- 关于电子温度依赖的原子间电位的配置原子温度的建议和应用,包括ab initio分子动力学.
- 在非热相过渡期间温度演变的研究.
主要成果:
- 动量子空间中的原子的动态温度不受电子激发的影响.
- 对于电子和原子温度不同的情况下,定义了一个配置原子温度.
- 经过超快辐射的固体表现出一种临时的多温度状态,具有明显的动量和配置平衡.
- 原子温度的完全平衡发生在较长的时间尺度上,导致能量均分.
结论:
- 这项研究为理解非平衡激发固体中的原子温度提供了理论框架.
- 拟议的配置温度对于电子刺激下的初始分子动力学等模拟至关重要.
- 识别临时的多温度状态需要开发先进的热传输模型.
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