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相关概念视频

Superconductor01:24

Superconductor

1.9K
A substance that reaches superconductivity, a state in which magnetic fields cannot penetrate, and there is no electrical resistance, is referred to as a superconductor. In 1911, Heike Kamerlingh Onnes of Leiden University, a Dutch physicist, observed a relation between the temperature and the resistance of the element mercury. The mercury sample was then cooled in liquid helium to study the linear dependence of resistance on temperature. It was observed that, as the temperature decreased, the...
1.9K
Atomic Nuclei: Nuclear Spin State Population Distribution01:14

Atomic Nuclei: Nuclear Spin State Population Distribution

2.4K
Near absolute zero temperatures, in the presence of a magnetic field, the majority of nuclei prefer the lower energy spin-up state to the higher energy spin-down state. As temperatures increase, the energy from thermal collisions distributes the spins more equally between the two states. The Boltzmann distribution equation gives the ratio of the number of spins predicted in the spin −½ (N−) and spin +½ (N+) states.
2.4K
Phase Transitions: Melting and Freezing02:39

Phase Transitions: Melting and Freezing

15.3K
Heating a crystalline solid increases the average energy of its atoms, molecules, or ions, and the solid gets hotter. At some point, the added energy becomes large enough to partially overcome the forces holding the molecules or ions of the solid in their fixed positions, and the solid begins the process of transitioning to the liquid state or melting. At this point, the temperature of the solid stops rising, despite the continual input of heat, and it remains constant until all of the solid is...
15.3K
Types Of Superconductors01:28

Types Of Superconductors

1.7K
A superconductor is a substance that offers zero resistance to the electric current when it drops below a critical temperature. Zero resistance is not the only interesting phenomenon as materials reach their transition temperatures. A second effect is the exclusion of magnetic fields. This is known as the Meissner effect. A light, permanent magnet placed over a superconducting sample will levitate in a stable position above the superconductor. High-speed trains that levitate on strong...
1.7K
Phase Transitions: Vaporization and Condensation02:39

Phase Transitions: Vaporization and Condensation

21.6K
The physical form of a substance changes on changing its temperature. For example, raising the temperature of a liquid causes the liquid to vaporize (convert into vapor). The process is called vaporization—a surface phenomenon. Vaporization occurs when the thermal motion of the molecules overcome the intermolecular forces, and the molecules (at the surface) escape into the gaseous state. When a liquid vaporizes in a closed container, gas molecules cannot escape. As these gas phase molecules...
21.6K
Phase Transitions: Sublimation and Deposition02:33

Phase Transitions: Sublimation and Deposition

20.4K
Some solids can transition directly into the gaseous state, bypassing the liquid state, via a process known as sublimation. At room temperature and standard pressure, a piece of dry ice (solid CO2) sublimes, appearing to gradually disappear without ever forming any liquid. Snow and ice sublimate at temperatures below the melting point of water, a slow process that may be accelerated by winds and the reduced atmospheric pressures at high altitudes. When solid iodine is warmed, the solid sublimes...
20.4K

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相关实验视频

Updated: Feb 18, 2026

Comparison of Two Different Synthesis Methods of Single Crystals of Superconducting Uranium Ditelluride
04:51

Comparison of Two Different Synthesis Methods of Single Crystals of Superconducting Uranium Ditelluride

Published on: July 8, 2021

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预测最大超冷却在SU(N) 限制过渡的预测.

Prateek Agrawal1,2, Gaurang Ramakant Kane1, Vazha Loladze1

  • 1University of Oxford, Rudolf Peierls Centre for Theoretical Physics, Parks Road, Oxford OX1 3PU, United Kingdom.

Physical review letters
|February 16, 2026
PubMed
概括

在SU(N) -米尔斯理论中的热封闭相变是第一阶段. 格子数据中的一个小系数表明不稳定性,预测有限的超冷却和抑制的引力波信号.

科学领域:

  • 高能物理学的高能物理学
  • 量子场理论是量子场理论.
  • 统计力学就是统计力学.

背景情况:

  • 在SU(N) -米尔斯理论中,热封闭相变是一个关键的现象.
  • 众所周知,这种过渡是N≥3的第一顺序,反弹动作缩放为N^2.2.

研究的目的:

  • 调查在格子数据中观察到的小系数对反弹动作的影响.
  • 了解这个系数的起源及其对相位过渡动态的影响.
  • 预测SU(N) 理论中的最大可实现的超冷却及其实验测试性.

主要方法:

  • 对SU(N) -米尔斯理论的格子数据的分析.
  • 利用柔软破碎的超对称-米尔斯模型的见解.
  • 关于解封相位不稳定性的理论研究.

主要成果:

  • 有证据表明,小系数源于在临界温度以下的解锁相位不稳定.
  • 在SU(N) 理论中,最大可实现的超冷却预计为几个百分比.
  • 有可能显著抑制相关的宇宙引力波信号.

结论:

  • 观察到的格子数据系数指向了一个特定的不稳定机制.

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  • 有限超冷的预测为网格模拟提供了可测试的假设.
  • 宇宙引力波信号可能比之前预期的要弱得多.