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超流体涡旋重连普遍性的实验与理论证据

Experimental and theoretical evidence of universality in superfluid vortex reconnections.

作者信息

Stasiak Piotr Z, Xing Yiming, Alihosseini Yousef, Barenghi Carlo F, Baggaley Andrew, Guo Wei, Galantucci Luca, Krstulovic Giorgio

机构信息

School of Mathematics, Statistics and Physics, Newcastle University, Newcastle upon Tyne NE1 7RU, United Kingdom.

National High Magnetic Field Laboratory, Tallahassee, FL 32310.

出版信息

Proc Natl Acad Sci U S A. 2025 May 27;122(21):e2426064122. doi: 10.1073/pnas.2426064122. Epub 2025 May 22.

DOI:10.1073/pnas.2426064122
PMID:40402248
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC12130869/
Abstract

The minimum separation between reconnecting vortices in fluids and superfluids obeys a universal scaling law with respect to time. The prereconnection and the postreconnection prefactors of this scaling law are different, a property related to irreversibility and to energy transfer and dissipation mechanisms. In the present work, we determine the temperature dependence of these prefactors in superfluid helium from experiments and a numeric model which fully accounts for the coupled dynamics of the superfluid vortex lines and the thermal normal fluid component. At all temperatures, we observe a pre- and postreconnection asymmetry similar to that observed in other superfluids and in classical viscous fluids, indicating that vortex reconnections display a universal behavior independent of the small-scale regularizing dynamics. We also numerically show that each vortex reconnection event represents a sudden injection of energy in the normal fluid. Finally we argue that in a turbulent flow, these punctuated energy injections can sustain the normal fluid in a perturbed state, provided that the density of superfluid vortices is large enough.

摘要

流体和超流体中重新连接的涡旋之间的最小间距随时间遵循普遍的标度律。该标度律的重连前和重连后预因子不同,这一特性与不可逆性以及能量转移和耗散机制有关。在本工作中,我们通过实验和一个完全考虑超流体涡旋线与热正常流体成分耦合动力学的数值模型,确定了这些预因子在超流氦中的温度依赖性。在所有温度下,我们观察到重连前后的不对称性,类似于在其他超流体和经典粘性流体中观察到的情况,这表明涡旋重连表现出与小尺度正则化动力学无关的普遍行为。我们还通过数值计算表明,每次涡旋重连事件都代表着向正常流体中突然注入能量。最后我们认为,在湍流中,只要超流体涡旋的密度足够大,这些间歇性的能量注入就能使正常流体维持在扰动状态。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6126/12130869/c6f3555f1aca/pnas.2426064122fig04.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6126/12130869/1e273643df15/pnas.2426064122fig01.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6126/12130869/77e340242f11/pnas.2426064122fig02.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6126/12130869/dd663bd6e27c/pnas.2426064122fig03.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6126/12130869/c6f3555f1aca/pnas.2426064122fig04.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6126/12130869/1e273643df15/pnas.2426064122fig01.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6126/12130869/77e340242f11/pnas.2426064122fig02.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6126/12130869/dd663bd6e27c/pnas.2426064122fig03.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6126/12130869/c6f3555f1aca/pnas.2426064122fig04.jpg

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本文引用的文献

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