在相调节周期结构中的危机诱导的振动共振
P O Adesina1, U E Vincent2, T O Roy-Layinde3
1Department of Physical Sciences, <a href="https://ror.org/01v0we819">Redeemer's University</a>, Ede 232102, Nigeria and Department of Physics, <a href="https://ror.org/03wx2rr30">University of Ibadan</a>, Ibadan, Nigeria.
Physical review. E
|October 19, 2024
概括
这项研究揭示了Josephson连接振荡器与相调节的双振荡共振. 研究人员确定了共振感应和放大,解释了双重共振现象.
科学领域:
- 非线性动力学是一种非线性动力学.
- 凝聚物质物理学 凝聚物质物理学
- 量子电子学 量子电子学
背景情况:
- 约瑟夫森连接在量子电子学中至关重要,在外部强迫下表现出复杂的动态.
- 了解驱动非线性系统中的共振现象是控制它们行为的关键.
研究的目的:
- 为了研究和解释在驱动的约瑟夫森交叉振荡器中发生的双振荡共振的发生.
- 为了确定负责观察到的双重共振的潜在机制.
主要方法:
- 带动振荡器模型的理论分析与高频相调节.
- 数字模拟以探索系统的动态和共振效应.
- 对相调节效应的分析,包括共振感应和放大.
主要成果:
- 在约瑟夫森交叉振荡器中观察并证实了双重振动共振.
- 确定了两个不同的相调节效应:共振诱导和共振放大.
- 通过吸引力融合危机将诱导的共振与从周期性到准周期性行为的过渡联系起来.
结论:
- 约瑟夫森连接处的双振共振是由特定的相调节效应驱动的.
- 过渡到准周期性和吸引力合并危机对于理解这种共振现象至关重要.
- 这项工作为控制和预测非线性振荡器中的复杂动态提供了洞察力.
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