在对称的零范围过程中的电流波动在临界密度以下和临界密度下
Tanmoy Chakraborty1, Punyabrata Pradhan1, Kavita Jain2
1Department of Physics of Complex Systems, <a href="https://ror.org/00kz6qq24">S. N. Bose National Centre for Basic Sciences</a>, Block-JD, Sector-III, Salt Lake, Kolkata 700106, India.
Physical review. E
|December 18, 2024
概括
这项研究分析了相位过渡附近的对称零范围过程中的电流波动. 我们发现,集成电流的方差随着时间的推移而增长,在远离和临界点时表现出不同的行为.
科学领域:
- 统计力学 统计力学
- 凝聚物质物理学 凝聚物质物理学
- 非平衡系统 非平衡系统
背景情况:
- 在稳定状态中描述当前波动至关重要,但通常仅限于非关键系统.
- 了解接近相位过渡的系统需要先进的分析技术.
研究的目的:
- 分析计算对称的零范围过程的传输系数,表现出相位过渡.
- 描述时间集成的电流在稳定状态和临界状态的波动.
主要方法:
- 分析计算密度依赖的传输系数 (批量扩散,粒子移动性).
- 水力动力缩放分析. 水力动力缩放分析.
- 缩放理论在临界点上的应用.
主要成果:
- 远离关键性,集成电流尺度的方差为 sqrt ((t) 在短时间和t在长时间.
- 导出一个完整的变量缩放函数,量化当前波动增长.
- 在临界度时,短期行为显示异常增长指数与模型参数不同.
结论:
- 该研究提供了对具有相位过渡的系统中电流波动的全面描述.
- 不同的缩放行为被识别在远离和在关键点.
- 这些发现提供了对非平衡统计力学和关键现象的见解.
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