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関連する概念動画

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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関連する実験動画

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

3.2K

SU(N) コンファインメント トランジションの最大超冷却の予測

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
まとめ

SU(N) ヤング・ミルズ理論における熱閉じ込め相変遷は,一等である. 格子データの小さな係数は不安定性を示唆し,限られた超冷却と抑制された重力波信号を予測する.

科学分野:

  • 高エネルギー物理学の物理学
  • 量子場論は量子場論である.
  • 統計学の力学 統計学の力学

背景:

  • SU(N) ヤング・ミルズ理論における熱収束相移行は,重要な現象である.
  • この移行は,N≥3のファーストオーダーで,ボunceアクションのスケーリングはN^2.2.として知られています.

研究 の 目的:

  • 格子データで観測された小さな係数の反発作用への影響を調査する.
  • この係数の起源と相変化の動態への影響を理解する.
  • SU(N) 理論で達成可能な最大超冷却と,その実験的検証性を予測する.

主な方法:

  • SU(N) ヤング・ミルズ理論のための格子データの分析.
  • 柔らかく折れた超対称的なヤング・ミルズモデルからの洞察を活用する.
  • デコンフィネッド・フェーズ・インスタビリティの理論的調査.

主要な成果:

  • 証拠によると,この小さな係数は,臨界温度を下回る段階の不安定性から生じるという.
  • SU(N) 理論で達成可能な最大超冷却は,数パーセントであると予測されています.
  • 関連する宇宙学的重力波信号を大幅に抑制する可能性がある.

さらに関連する動画

Setting Limits on Supersymmetry Using Simplified Models
07:46

Setting Limits on Supersymmetry Using Simplified Models

Published on: November 15, 2013

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Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving
11:21

Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving

Published on: March 30, 2017

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関連する実験動画

Last 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

3.2K
Setting Limits on Supersymmetry Using Simplified Models
07:46

Setting Limits on Supersymmetry Using Simplified Models

Published on: November 15, 2013

9.0K
Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving
11:21

Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving

Published on: March 30, 2017

7.9K

結論:

  • 観測された格子データ係数は,特定の不安定性メカニズムを示しています.
  • 限られた超冷却の予測は,格子シミュレーションのためのテスト可能な仮説を提供します.
  • 宇宙学的重力波の信号は,これまで予想されていたよりもかなり弱くなっている可能性があります.